Microwave integrated quantum circuits with cap wafers and their methods of manufacture

ABSTRACT

In a general aspect, an integrated quantum circuit includes a first substrate and a second substrate. The first substrate includes a first surface and a recess formed in the first substrate along the first surface. The recess has a recess surface and is configured to enclose a quantum circuit element. The first substrate includes a first electrically-conductive layer disposed on the first surface and covering at least a portion of the recess surface. The first electrically-conductive layer includes a first superconducting material. The second substrate includes a second surface and a quantum circuit element. The second substrate includes a second electrically-conductive layer on the second surface that includes a second superconducting material. The first substrate is adjacent the second substrate to enclose the quantum circuit device within the recess. The first electrically-conductive layer of the first substrate is electrically-coupled to the second electrically-coupled layer of the second substrate.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application claims priority to U.S. Provisional Application Ser. No. 62/521,888 entitled “Microwave Integrated Quantum Circuits with Cap Wafer and Methods for Making the Same”, filed Jun. 19, 2017. The disclosure of the priority application is hereby incorporated herein by reference.

BACKGROUND

The following description relates to quantum circuits, and more particularly, to quantum circuits enclosed by cap wafers.

Quantum computers can perform computational tasks by executing quantum algorithms. In some quantum computing architectures, quantum algorithms are executed on superconducting qubits that are subject to noise. The superconducting qubits can be implemented, for example, using circuits that include Josephson-junctions.

DESCRIPTION OF DRAWINGS

FIG. 1 is a block diagram of a quantum computing system.

FIG. 2A shows an equivalent circuit of a portion of a microwave integrated quantum circuit.

FIG. 2B shows a two dimensional (2D) microwave integrated quantum circuit that includes a circuit wafer.

FIGS. 3A-3D show aspects of a 2D microwave integrated quantum circuit that includes a circuit wafer and a cap wafer.

FIGS. 4A-4D show aspects of a 2D microwave integrated quantum circuit that includes a circuit wafer and two cap wafers of a single type.

FIG. 4E shows a three dimensional (3D) microwave integrated quantum circuit that includes multiple circuit wafers and cap wafers of two types.

FIGS. 5A-5C show aspects of a 2D microwave integrated quantum circuit that includes a circuit wafer and thru vias.

FIGS. 6A-6D show aspects of 2D microwave integrated quantum circuits that include a circuit wafer, thru vias, and one or more cap wafers of a single type.

FIG. 6E shows a 3D microwave integrated quantum circuit that includes circuit wafers and cap wafers of multiple types, and thru vias.

FIG. 6F shows a 3D microwave integrated quantum circuit that includes multiple circuit wafers and cap wafers of a single type, and thru vias.

FIGS. 7A-7D show aspects of multiple types of thru vias.

FIG. 8 shows an example of a process for fabricating either of circuit wafers or routing wafers based on etching.

FIG. 9 shows an example of a process for fabricating cap wafers using wet etching of Si wafers.

FIG. 10 shows an example of a process for fabricating cap wafers using wet etching of Si on insulator (SOI) wafers.

FIG. 11A shows an example of a process for fabricating cap wafers using deep reactive-ion etching (DRIE) of Si wafers.

FIGS. 11B-11C show an example of a process that uses SU-8 as structural material for fabricating cap wafers.

FIG. 12 shows an example of a process for fabricating cap wafers that are coated with an electrically conductive layer and have In bumps.

FIGS. 13A-13B show an example of a process for fabricating circuit wafers that have thru vias.

FIG. 14A shows an example of a process for bonding constitutive wafers of a 2D microwave integrated quantum circuit using In bumps at low temperature.

FIG. 14B shows aspects of a process for bonding constitutive wafers of a 3D microwave integrated quantum circuit using In bumps at low temperature.

FIG. 15 shows an example of a process for bonding constitutive wafers of a 2D microwave integrated quantum circuit using In balls at low temperature.

FIG. 16 shows an example of a process for bonding constitutive wafers of a 2D microwave integrated quantum circuit using solder reflow at low temperature.

FIG. 17A shows a 2D microwave integrated quantum circuit that includes a circuit wafer and two cap wafers that have mating features that are distal to quantum circuit devices thereof.

FIGS. 17B-17C show an example of a process for fabricating the cap wafers with mating features.

FIG. 18 shows a 2D microwave integrated quantum circuit that includes a circuit wafer and two cap wafers that have mating features that are adjacent to quantum circuit devices thereof.

FIG. 19 shows a quantum computing apparatus that includes a quantum computing device and an interposer.

FIGS. 20A and 20B show examples of quantum computing devices with patterned metal layers on their back surfaces for bonding to an interposer.

FIG. 21 shows an example of a quantum computing apparatus having a multilayer interposer including various integrated circuit layers and a connectorization layer.

FIG. 22 shows an example of a quantum computing apparatus having an interposer that includes a ceramic layer attached to a circuit wafer by indium bonding.

FIG. 23 shows an example of a quantum computing apparatus having a multilayer interposer attached to a circuit wafer by wire bonding.

FIG. 24 shows an example of a quantum computing apparatus having a multilayer silicon interposer attached to a circuit wafer by indium bonding.

FIG. 25 shows an example of a quantum computing apparatus having a multilayer interposer that includes a thinnerposer.

FIG. 26 shows an example of a quantum computing apparatus having a multilayer interposer including silicon layers attached by aluminum bonding.

FIG. 27 shows an example of a quantum computing apparatus including integrated circuit layers formed on the back surface of a circuit wafer.

FIG. 28 is a schematic diagram of example multi-layer material stacks on an example cap wafer and circuit wafer.

DETAILED DESCRIPTION

Technologies are described for constructing and packaging microwave integrated quantum circuits to be used in quantum computing systems. Prior to describing example implementations of techniques for constructing and packaging microwave integrated quantum circuits, structural aspects and functional aspects of a quantum computing system are described.

FIG. 1 shows an example of a quantum computing system 100. The quantum computing system 100 includes a control system 110, a signal delivery system 106, and a quantum processor cell 102. More generally, quantum computing systems may include additional or different features, and the components of a quantum computing system may operate as described with respect to FIG. 1 or in another manner.

The quantum computing system 100 shown in FIG. 1 can perform quantum computational tasks by executing quantum algorithms (e.g., step-by-step procedures for solving a problem on a quantum computer). In some implementations, the quantum computing system 100 can perform quantum computation by storing and manipulating information within individual quantum states of a composite quantum system. For example, qubits (i.e., quantum bits) can be stored in and represented by an effective two-level sub-manifold of a quantum coherent physical system. Coupler devices can be used to perform quantum logic operations on single qubits or conditional quantum logic operations on multiple qubits. In some instances, the conditional quantum logic can be performed in a manner that allows large-scale entanglement within the quantum computing device. Control signals can manipulate the quantum states of individual qubits and the joint states of multiple qubits. In some instances, information can be read out from the composite quantum system by measuring the quantum states of the individual qubits.

In some implementations, the quantum computing system 100 can operate using gate-based models for quantum computing. In some models, fault-tolerance can be achieved by applying a set of high-fidelity control and measurement operations to the qubits. For example, topological quantum error correction schemes can operate on a lattice of nearest-neighbor-coupled qubits. In some instances, these and other types of quantum error correcting schemes can be adapted for a two- or three-dimensional lattice of nearest-neighbor-coupled qubits, for example, to achieve fault-tolerant quantum computation. The lattice can allow each qubit to be independently controlled and measured without introducing errors on other qubits in the lattice. Adjacent pairs of qubits in the lattice can be addressed, for example, with two-qubit gate operations that are capable of generating entanglement, independent of other pairs in the lattice.

In some implementations, the quantum computing system 100 is constructed and operated according to a scalable quantum computing architecture. For example, in some cases, the architecture can be scaled to a large number of qubits to achieve large-scale general purpose coherent quantum computing. In some instances, the architecture is adaptable and can incorporate a variety of modes for each technical component. For example, the architecture can be adapted to incorporate different types of qubit devices, coupler devices, readout devices, signaling devices, etc.

The quantum processor cell 102 includes qubit devices that are used to store and process quantum information. In some instances, all or part of the quantum processor cell 102 functions as a quantum processor, a quantum memory, or another type of subsystem. The quantum processor cell 102 can be implemented, for example, based on the examples described below or in another manner.

In the quantum processor cell 102, the qubit devices each store a single qubit (a bit of quantum information), and the qubits can collectively define the computational state of a quantum processor or quantum memory. The quantum processor cell 102 may also include readout devices that selectively interact with the qubit devices to detect their quantum states. For example, the readout devices may generate readout signals that indicate the computational state of the quantum processor or quantum memory. The quantum processor cell 102 may also include coupler devices that selectively operate on individual qubits or pairs of qubits. For example, the coupler devices may produce entanglement or other multi-qubit states over two or more qubits in the quantum processor cell 102.

In some implementations, the quantum processor cell 102 processes the quantum information stored in the qubit devices by applying control signals to the qubit devices or to the coupler devices housed in the quantum processor cell. The control signals can be configured to encode information in the qubit devices, to process the information by performing logical gates or other types of operations, or to extract information from the qubit devices. In some examples, the operations can be expressed as single-qubit gates, two-qubit gates, or other types of logical gates that operate on one or more qubit devices. A sequence of operations can be applied to the qubit devices to perform a quantum algorithm. The quantum algorithm may correspond to a computational task, a quantum error correction procedure, a quantum state distillation procedure, or a combination of these and other types of operations.

The signal delivery system 106 provides communication between the control system 110 and the quantum processor cell 102. For example, the signal delivery system 106 can receive control signals (e.g., qubit control signals, readout control signals, coupler control signals, etc.) from the control system 110 and deliver the control signals to the quantum processor cell 102. In some instances, the signal delivery system 106 performs preprocessing, signal conditioning, or other operations to the control signals before delivering them to the quantum processor cell 102. In many instances, the signal delivery system 106 includes an interposer which provides electrical connections between the quantum processor cell 102 and cables (or other signal lines) to the control system 110.

The control system 110 controls operation of the quantum processor cell 102. The control system 110 may include data processors, signal generators, interface components and other types of systems or subsystems. In some cases, the control system 110 includes one or more classical computers or classical computing components.

Various implementations of the quantum processor cell 102 are described below, including various embodiments of its components along with various methods for fabricating the quantum processor cell and its components.

While generally the quantum processor cell 102 can be implemented using a variety of different qubit devices, readout devices, and coupler devices, FIG. 2A shows an equivalent circuit of an example of a microwave integrated quantum circuit 148 that can be used to perform quantum operations. Here, the microwave integrated quantum circuit 148 includes a subset of qubit devices 144, their corresponding readout devices 146 and a subset of the coupler devices 142 from the quantum processor cell 102. In this example, the microwave integrated quantum circuit 148 includes qubit devices 144-j and 144-(j+1), corresponding readout devices 146-j and 146-(j+1), and a tunable coupler device 142-(j,j+1) disposed between the qubit devices 144-j and 144-(j+1). In the example shown in FIG. 2A, each of the qubit devices 144-j and 144-(j+1) is capacitively coupled to the coupler device 142-(j,j+1) by respective differential capacitances 150-j and 150-(j+1). Also, each of the qubit devices 144-j and 144-(j+1) is capacitively coupled to its respective readout device 146-j and 146-(j,j+1) by respective differential capacitances 152-j and 152-(j+1).

Write signals (e.g., coupler control signals, qubit control signals, readout control signals, etc.) can be transmitted from the control system 110, through the signal delivery system 106, to various input ports of the microwave integrated quantum circuit 148. An example of such input port is shown in FIG. 2A as a coupler control input port 154-(j,j+1). In this manner, the tunable coupler device 142-(j,j+1) is inductively coupled with a source of coupler control signals at the coupler control input port 154-(j,j+1). Other examples of input ports are shown in FIG. 2A as qubit+readout control port 156-j and qubit+readout control port 156-(j+1). In this manner, each of the readout devices 146-j and 146-j+1 is capacitively coupled to a source of qubit control signals and a source of readout control signals at the respective qubit+readout control ports 156-j and 156-(j+1). Additionally, readout signals (e.g., qubit readout signals) are received by the control system 110 through the system delivery system 106 and from various output ports in the microwave integrated quantum circuit 148. In the example microwave integrated quantum circuit 148 shown in FIG. 2A, the qubit+readout control ports 156-j and 156-(j+1) also are used as output ports. Note that the control signals and the readout signals used to operate the quantum circuit devices of the microwave integrated quantum circuit 148 and of other microwave integrated quantum circuits disclosed in this specification have frequencies in the microwave frequency range. As such, the term operating frequency (i.e., f₀) of a quantum circuit device, as used in this specification, represents a microwave frequency of a control signal or a readout signal used to operate quantum circuit devices of a microwave integrated quantum circuits disclosed in this specification.

Each of the qubit devices 144-j, 144-(j+1) includes a Josephson junction (represented by the symbol “X” in FIG. 2A) and a shunt capacitance. Qubit devices 144-j, 144-(j+1) can be implemented as transmon qubits, as flux qubits or as fluxonium qubits, as described in connection with FIG. 3B of PCT application publication WO 2015/178990, the content of which is incorporated herein by reference. In the example shown in FIG. 2A, the tunable coupler device 142-(j,j+1) includes a Josephson junction (represented by the symbol “X” in FIG. 2A), a shunt inductance and a shunt capacitance. A tunable coupler device 142 can be implemented as a fluxonium coupler 170, as described in connection with FIG. 3B of PCT application publication WO 2015/178990.

The portion of the microwave integrated quantum circuit 148 illustrated in FIG. 2A can be copied multiple times, e.g., as a unit cell, to extend the microwave integrated quantum circuit 148 along a path (e.g., along x-axis of a Cartesian coordinate system), on a surface (e.g., x-y plane of a Cartesian coordinate system) or in space (e.g., as layers parallel to x-y plane that are distributed along a z-axis of a Cartesian coordinate system). For example, fault-tolerance quantum computing can be achieved by implementing gate-based models in a two-dimensional (2D) microwave integrated quantum circuit 148 that includes a large number of nearest-neighbor coupled qubit devices 144. A 2D microwave integrated quantum circuit 148 can allow each qubit device 144 to be independently controlled and measured without introducing crosstalk or errors on other qubit devices 144 in the 2D microwave integrated quantum circuit. Nearest-neighbor pairs of qubit devices 144 in the 2D microwave integrated quantum circuit 148 should be addressable with two-qubit gate operations capable of generating entanglement, independent of all other such pairs in the 2D microwave integrated quantum circuit 148. Exemplary implementations of 2D microwave integrated quantum circuits 200, 300, 400, 500, 600A, 600B are described below in relation to respective FIGS. 2B, 3A, 4A, 5A, 6A, 6B. As another example, fault-tolerant quantum computing can likewise be performed in a three-dimensional (3D) microwave integrated quantum circuit 148M that includes a large number of nearest-neighbor coupled qubit devices 144. Exemplary implementations of 3D microwave integrated quantum circuits 400M, 600AM, 600BM are described below in relation to respective FIGS. 4E, 6E, 6F.

A variety of technical features may be used (alone or in combination) in microwave integrated quantum circuits to carry out large-scale, fault tolerant quantum computing. One such feature is the delivery of control signals to qubit devices 144 and tunable coupling devices 142 of a 2D microwave integrated quantum circuit 148 or a 3D microwave integrated quantum circuit 148, and another such feature is the extraction of measurement signals from the qubit devices 144 being performed with low-crosstalk of the applied signals from target qubit devices to non-target qubit devices. Another such feature is the ability to sustain coherence of individual and entangled quantum states of the qubit devices 144 of the 2D microwave integrated quantum circuit 148 or the 3D microwave integrated quantum circuit 148. Yet another such feature is the shielding and isolation of the qubit device 144-j from external noise, from the external environment, and from each other qubit device 144-(j+k) in the 2D microwave integrated quantum circuit 148 or the 3D microwave integrated quantum circuit 148 to which the qubit device 144-j is not specifically coupled (k≠0 or ±1) for performing a two-qubit gate.

For instance, FIG. 2B shows a 2D microwave integrated quantum circuit 200, similar to the microwave integrated quantum circuit 148, including quantum circuit devices 240 fabricated on a first substrate 210. As the first substrate supports the quantum circuit devices 240, it will also be referred to as the circuit wafer 210. Microwave signals may be used to operate each of the quantum circuit devices 240 of 2D microwave integrated quantum circuit 200. In this example, such microwave signals can propagate to nearest-neighbor quantum circuit devices (and beyond) by the appearance of an in-air electric field spatial distribution (i.e., E_(air)) and an in-substrate electric field spatial distribution (i.e., E_(sub)) of the operating signals, as shown in FIG. 2B. Additionally, the quantum circuit devices 240 of the 2D microwave integrated quantum circuit 200 may be exposed to the external electromagnetic environment.

In some implementations, the quantum circuit devices 240 can be isolated (e.g., exponentially) from each other using one encapsulation substrate or a pair of encapsulation substrates lined with an electrically conducting layer that is grounded during operation of the microwave integrated quantum circuits (e.g., see 2D microwave integrated quantum circuits 300, 400 and 3D microwave integrated quantum circuit 400M, described below). In some implementations, the electrically conducting layer includes a multi-layer material stack. The multi-layer material stack may include one or more layers of superconducting material and one or more layers of non-superconducting material (e.g., palladium), while maintaining one or more superconducting properties. Here, recesses of the encapsulation substrates are sized to cause available modes of the recesses to evanesce with respect to relevant operating frequencies of the encapsulated quantum circuit devices 240. In certain implementations, the quantum circuit devices 240 can be isolated from each other using electrically conducting thru vias formed in the circuit wafer 210 of the 2D microwave integrated quantum circuit, where the electrically conducting thru vias are grounded during operation of the microwave integrated quantum circuit (e.g., see 2D microwave integrated quantum circuit 500, described below). Here, the electrically-conducting thru vias are distributed around a respective footprint of each quantum circuit device 240 to cause available modes of the electrically conducting thru via distribution to evanesce with respect to relevant operating frequencies of the surrounded quantum circuit device. In some implementations, a combination of an encapsulation substrate and electrically-conducting thru vias so-distributed is used to isolate the quantum circuit devices 240 from each other (e.g., see 2D microwave integrated quantum circuits 600A, 600B, and 3D microwave integrated quantum circuits 600AM, 600BM, described below). In this manner, the quantum circuit devices 240 can be shielded and isolated from their nearest neighbors and from the external electromagnetic environment.

FIG. 3A is a side view of a 2D microwave integrated quantum circuit 300, and FIG. 3B is a top view of the same circuit in the vicinity of one of a plurality of quantum circuit devices 240 included in the 2D microwave integrated quantum circuit. Here, the 2D microwave integrated quantum circuit 300 includes a first substrate 210, also referred to as a circuit wafer, such that the quantum circuit devices 240 are disposed on a first surface of the circuit wafer 210. Each quantum circuit device QC-j 240, where j=1, 2, 3, . . . , has an associated operating frequency f₀-j. In some implementations, the operating frequencies of the quantum circuit devices 240 are different from each other. In other implementations, at least some of the quantum circuit devices 240 have common operating frequencies.

The 2D microwave integrated quantum circuit 300 further includes a second substrate 310 having a first surface that defines recesses 320 of the second substrate that correspond to the quantum circuit devices 240 disposed on the circuit wafer 210. In this manner, the circuit wafer 210 and second substrate 310 are arranged such that each recess 320 of the second substrate forms an enclosure that houses a respective quantum circuit device 240. A dimension C_(h), e.g., along the z-axis, of each recess 320 can range from 5 μm-500 μm (e.g., 20 μm-200 μm) for a thickness of the second substrate 210 in a range from 1 μm to 1 mm. As the second substrate 310 “caps” the quantum circuit devices 240 disposed on the circuit wafer 210, the second substrate will be referred to as the cap wafer 310. Note that the cap wafer 310 is bonded to the circuit wafer 210, as described below in relation to FIGS. 14A-14B, 15 and 16. In addition, spacers (or standoff bumps) may be used between the bonded cap wafer 310 and the circuit wafer 210, as described below in relation to FIGS. 12, 13A-13B, 14A-14B, 15 and 16.

Additionally, the 2D microwave integrated quantum circuit 300 includes an electrically conducting layer 350 that covers at least a portion of each of the recesses 320 of the cap wafer 310. In some implementations, the electrically conducting layer 350 includes a material (e.g., Al, In, Ti, Pn, Sn, etc.) that is superconducting at an operating temperature of the 2D microwave integrated quantum circuit 300. In other implementations, the electrically conducting layer 350 includes a material that has normal conductance (i.e., it is an electrical conductor but not superconducting) at the operating temperature of the 2D microwave integrated quantum circuit 300. In this manner, the 2D microwave integrated quantum circuit 300 can be operated at cryogenic temperatures (e.g., using liquid helium) and the electrically conducting layer 350 (or at least a portion thereof) can operate as a superconducting layer at that temperature. In addition, during operation of the 2D microwave integrated quantum circuit 300, the electrically conducting layer 350 is grounded. Although illustrated as one layer in FIG. 3A, in some implementations, the electrically conducting layer 350 includes a multi-layer material stack. For example, the electrically conducting layer 350 may include a stack similar to the stacks 2811, 2821 described below with respect to FIG. 28. In some instances, one or more layers of the multi-layer material stack include a superconducting material. In some instances, one or more layers of the multi-layer material stack include a non-superconducting material (e.g., palladium, platinum, or gold), but the multi-layer material stack may maintain one or more superconducting properties. For example, despite containing a non-superconducting material, the multi-layer material stack may exhibit a zero or near-zero resistance (e.g., less than one milli-ohm).

Moreover, each recess 320 is configured (e.g., sized) to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below a cutoff frequency f_(C), (i.e., f<f_(C)), where the cutoff frequency f_(C) is larger than the operating frequency f₀, (i.e., f₀<f_(C)) of the respective encapsulated quantum circuit device 240. The noted suppression of the propagation of the recess modes is illustrated in FIG. 3A by the relative appearance of the in-air electric field spatial distribution (i.e., E_(air)) and the in-substrate electric field spatial distribution (i.e., E_(sub)) of operating signals. Note that because the cutoff frequency f_(C) is larger than the operating frequency f₀, the enclosure formed by the recess 320 is a non-resonant cavity relative to operation of the encapsulated quantum circuit device 240.

In this manner, a lateral dimension WW of a recess 320 is smaller than a maximum distance LMAX corresponding to the cutoff frequency f_(C). For example, the lateral dimension WW of a recess 320 can be range from 20 μm to 2 mm. Additionally, a distance DW between the outer perimeter of the encapsulated quantum circuit device 240 and a nearest wall of the recess 320 corresponds to a value of a capacitance between the encapsulated quantum circuit device and the portion of the electrically conducting layer 350 that covers the wall of the recess.

Moreover, adjacent quantum circuit devices 240 disposed on the circuit wafer 210 can be coupled electromagnetically through a coupling line that includes an electrical conductor 241 extending along the first surface of the circuit wafer over at least a portion of the distance between the adjacent quantum circuit devices. The coupling between the adjacent quantum circuit devices 240 can be capacitive or direct. Note that at least a portion of the coupling line is encapsulated by a trench 321 of the cap wafer 310, as illustrated in FIG. 3B.

The use of the cap wafer 310 can improve coherence times of the quantum circuit devices 240 disposed on the circuit wafer 210. Quantum circuit devices 240 with long coherence times are useful for the realization of a robust quantum processor cell 106. The cap wafer 310 can improve coherence times of the quantum circuit devices 240 of the 2D microwave integrated quantum circuit 300 relative to the 2D microwave integrated quantum circuit 200. Such improvement can include decreasing the participation ratio of the circuit wafer 210 (which is lossy at microwave frequencies) and increasing that of the air (which is lossless) so that more of the field resides in air. To estimate the improvement in coherence time due to cap wafer 310 we consider a dimension Co of the recess 320 of the cap wafer 310 on top of a silicon circuit wafer 210 of a given thickness. The participation ratios of the substrate Psub and air Pair are defined as

$\begin{matrix} {P_{air} = \frac{E_{air}}{E_{air} + E_{sub}}} & (1) \\ {P_{air} = \frac{E_{sub}}{E_{air} + E_{sub}}} & (2) \end{matrix}$ where E_(air)=∫dvϵ_(air)|E_(air)|² and E_(sub)=∫dvϵ_(sub)|E_(sub)|² are energies stored, respectively in the electric field in air (i.e., E_(air)) and in the circuit wafer 210 (i.e., E_(sub)).

The loss in the circuit wafer 210 can be described by the quality factor, Q_(Σ). In general, the dissipation factor (the loss-rate of energy) is related to the tangent δ via

$\begin{matrix} {\frac{1}{Q_{\Sigma}} = {\sum\limits_{j}{P_{j}\tan\;\delta_{j}}}} & (3) \end{matrix}$

The coherence time T₁ can be expressed in terms of the quality factor as

$\begin{matrix} {T_{1} = {\frac{Q_{\Sigma}}{\omega} = \frac{1}{\omega P_{sub}\tan\;\delta_{sub}}}} & (4) \end{matrix}$ where ω is the operating frequency of a quantum circuit device 240.

The participation ratio of air can be increased by tuning the dimension Co of the recess 320 of the cap wafer 310 as compared to the thickness of the circuit wafer 210. Simulations show that a more concentrated field in air is observed when the dimension Co of the recess 320 is smaller than the thickness of the circuit wafer 210.

FIG. 3C is a plot 301 that shows that, for a thickness of 100 μm for the circuit wafer 210, the participation ratio of the circuit wafer decreases as the dimension Co of the recess 320 of the cap wafer 310 decreases. This effect is substantial when the dimension Co of the recess 320 is below 50 μm. Note that the dimension Co of the recess 320 cannot be decreased indefinitely due to the possibility of other undesired effects, such as surface loss.

FIG. 3D is a plot 303 that shows a dependence of the coherence time T₁ on a dimension Co of the recess 320 of the cap wafer 310. The dependence is illustrated for multiple operating frequencies (i.e., f₀) of the quantum circuit devices 240, which is enclosed by the recess 320. A comparison of plots 301 and 303 suggests that the coherence time T₁ increases as the participation ratio of the circuit wafer 210 decreases. The participation ratio of air can be further improved by sandwiching the circuit wafer 210 between a pair of cap wafers, as described below.

FIG. 4A is a side view of a 2D microwave integrated quantum circuit 400 that includes a third substrate 410 (also referred to as a second cap wafer) in addition to the circuit wafer 210 that supports on its first surface the quantum circuit devices 240 and the cap wafer 310 described above in connection with FIGS. 3A-3B. The second cap wafer 410 has a first surface that defines recesses 420 of the third substrate that also correspond to the quantum circuit devices 240 disposed on the circuit wafer 210. Here, the circuit wafer 210 is sandwiched between the cap wafer 310 and the second cap wafer 410. Moreover, the cap wafer 310 and the second cap wafer 410 are arranged such that each recess 420 of the second cap wafer 410 and a back surface of the circuit wafer 210 form an enclosure that registers with a respective recess 320. The recess 320 houses an associated quantum circuit device 240. Note that the second cap wafer 410 is bonded to the circuit wafer 210, as described below in connection with FIGS. 15 & 16. In addition, spacers (or standoff bumps) may be used between the bonded cap wafer 310 and circuit wafer 210, as described below in relation to FIGS. 12, 13A-13B, 15 and 16.

Additionally, the 2D microwave integrated quantum circuit 400 includes an electrically-conducting layer 450 that covers at least a portion of each of the recesses 420 of the second cap wafer 410. In some implementations, the electrically conducting layer 450 includes a material (e.g., Al, In, Ti, Pn, Sn, etc.) that is superconducting at an operating temperature of the 2D microwave integrated quantum circuit 400. In other implementations, the electrically conducting layer 450 includes a material that has a normal conductance (i.e., it is electrically conducting but not superconducting) at the operating temperature of the 2D microwave integrated quantum circuit 400. In this manner, the 2D microwave integrated quantum circuit 400 can be operated at cryogenic temperatures (e.g., using liquid helium) and the electrically-conducting layer 450 (or at least a portion thereof) can operate as a superconducting layer at that temperature. In addition, during operation of the 2D microwave integrated quantum circuit 400, both electrically-conducting layers 350 and 450 are grounded. Although illustrated as one layer in FIG. 4A, in some implementations, the electrically-conducting layer 450 includes a multi-layer material stack. For example, the electrically conducting layer 450 may include a stack similar to the stacks 2811, 2821 described below in relation to FIG. 28. In some instances, one or more layers of the multi-layer material stack include a superconducting material. In some instances, one or more layers of the multi-layer material stack include a non-superconducting material (e.g., palladium, platinum, or gold), but the multi-layer material stack may maintain one or more superconducting properties. For example, despite containing a non-superconducting material, the multi-layer material stack may exhibit a zero or near-zero resistance (e.g., less than one milli-ohm).

Moreover, each recess 420 is configured (e.g., sized) to suppress propagation of electromagnetic waves that have frequencies “f” below the cutoff frequency f_(C) (i.e., f<f_(C)). Such suppression may occur inside the recess and across a volume of the circuit wafer 210 that is sandwiched between the recesses 320 and 420. The noted propagation suppression of the recess modes and of the substrate modes is illustrated in FIG. 4A by the relative appearance of an in-air electric field spatial distribution (i.e., E_(air)) and an in-substrate electric field spatial distribution (i.e., E_(sub)) of operating signals. Note that because the cutoff frequency f_(C) is larger than the operating frequency f₀, the enclosure formed by the recess 420 also is a non-resonant cavity relative to operation of the quantum circuit device 240 encapsulated in the non-resonant cavity formed by the recess 320.

Performance of the quantum circuit devices 240 of the 2D microwave integrated quantum circuit 400 can improve relative to the 2D microwave integrated quantum circuit 300 in the following manner. A participation ratio of the 2D microwave integrated quantum circuit 400 is given by

$\begin{matrix} {P_{k} = \frac{E_{k}}{E_{{air},1} + E_{{air},2} + E_{sub}}} & (5) \end{matrix}$ here E_(air,1)=∫dVϵ_(air,1)|E_(air,1)|², E_(air,1)=∫dVϵ_(air,1)|E_(air,1)|², and E_(sub)=∫dvϵ_(sub)|E_(sub)|² are energies stored in the electric field in air (i.e., E_(air,1)) confined by the top recess 320, electric field in air (i.e., E_(air,2)) confined by the bottom recess 420, and electric field confined in the circuit wafer 210, respectively.

The participation ratio of the circuit wafer 210, in general, increases as its thickness increases. For example, for a fixed C_(h) dimension of the top recess 320 and the bottom recess 320 of 100 μm, the participation ratio of the circuit wafer 210 can be as low as 70% for a circuit wafer of thickness 100 μm. FIG. 4B is a plot 401 that shows that the participation ratio goes up to 90% when the thickness of the circuit wafer 210 is increased to 500 μm. This increase is because, when the circuit wafer 210 is thick, most of the electric field emitted by the enclosed quantum circuit device 240 will be stored in the substrate.

Note that the participation ratio strongly depends on the dimension C_(h) of the top and bottom recesses 320 and 420. The smaller the dimension C_(h) of the top recess 320, the larger the participation ratio of air, and the smaller the participation ratio of the circuit wafer 210. FIG. 4C is a plot 403 that shows that, fixing the thickness of the circuit wafer 210 at 100 μm (a minimum thickness such that the circuit wafer is mechanically robust and reasonable to handle in microfabrication processes), the participation ratio of the circuit wafer can go below 50% for a dimension C_(h) of the top recess 320 of less than 50 μm and a dimension C_(h) of the bottom recess 420 of 500 μm. In fact, the participation ratio of the circuit wafer 210 can be significantly reduced by using dimensions C_(h) of the top and bottom recesses 320, 420 less than 50 μm along with a thin (less than 200 μm) thick circuit wafer 210. It is therefore beneficial to use two cap wafers 310, 410 to decrease the participation ratio of circuit wafer 210, albeit fabrication and bonding subtleties. Alternatively, the thickness of the circuit wafer 210 can be extremely thin (e.g., less than 10 μm) to reduce or minimize the participation ratio of the circuit wafer. Such a 2D microwave integrated quantum circuit can be fabricated on a thin membrane made of a low-loss material such as high-quality silicon oxide or silicon nitride substrates.

FIG. 4D is a top view of either the 2D microwave integrated quantum circuit 300 or the 2D microwave integrated quantum circuit 400. Here, it is shown that the 2D microwave integrated quantum circuit 300, 400 can be scaled to a large number of quantum circuit devices 240 that include multiple qubits 144, resonators 146, 148, tunable couplers 142, and so forth. Here, distances between adjacent qubits 144 can range from 0.5 mm to 5 mm, for instance. Note that recesses 320 of the (top) cap wafer 310 enclose each quantum circuit device 240 formed on the circuit wafer 210 and trenches 321 (which are recesses with large aspect ratio) of the (top) cap wafer enclose the coupling lines 241. Further note that in the case of 2D microwave integrated quantum circuit 400, the contours representing the recess walls can be the common footprint of the recesses 320 of the top cap wafer 310 and the recesses 420 of the bottom cap wafer 410.

FIG. 4E is a side view of a 3D microwave integrated quantum circuit 400M that includes multiple 2D microwave integrated quantum circuits similar to the microwave integrated quantum circuit 400. The outermost layers of the 3D microwave integrated quantum circuit 400M are the cap wafer 310 and the second cap wafer 410 that have been described above in relation to FIGS. 3A & 4A, respectively. Further, the 3D microwave integrated quantum circuit 400M includes multiple circuit wafers 210 stacked along the z-axis, each of the circuit wafers supporting a plurality of quantum circuit devices 240. For instance, quantum circuit devices QC1, QC2, QC3 are disposed on a first circuit wafer 210, quantum circuit devices QC4, QC5, QC6 are disposed on a second circuit wafer 210, and so forth. In this manner, a given quantum circuit device 240, e.g., QC2, has a particular number of near-neighbor quantum circuit devices disposed on the same circuit wafer 210, e.g., some of which are QC1 and QC3, and one or two near-neighbor quantum circuit devices disposed on respective one or two adjacent circuit wafers, e.g., QC5. Moreover, each quantum circuit device QC-j 240, where j=1, 2, 3, 4, 5, 6, . . . , has an associated operating frequency f₀-j. In some implementations, the operating frequencies of adjacent quantum circuit devices 240 are different from each other. In other implementations, at least some of the adjacent quantum circuit devices 240, whether in-plane or out-of-plane, have common operating frequencies.

Note that adjacent instances of the multiple stacked circuit wafers 210 are separated by another type of cap wafer referred to as a bottom or top cap wafer 430. The bottom or top cap wafer 430 has a first surface that defines recesses 420 corresponding to the recesses 420 of the bottom cap wafer 410, and a second, opposing surface that defines recesses 320 corresponding to the recesses 320 of the top cap wafer 310. Here, the recesses 420 of the bottom or top cap wafer 430 correspond to the quantum circuit devices 240 disposed on the circuit wafer 210 adjacent to the first surface of the bottom or top cap wafer. Similarly, the recesses 320 of the bottom or top cap wafer 430 correspond to the quantum circuit devices 240 disposed on the circuit wafer 210 adjacent to the second surface of the bottom or top cap wafer. Note that the bottom or top cap wafer 430 is bonded to each of adjacent circuit wafers 210, as described below in relation to FIGS. 14A-14B, 15 and 16. In addition, spacers (or standoff bumps) may be used between the bonded bottom or top cap wafer 430 and each of adjacent circuit wafers 210, as described below in relation to FIGS. 12, 13A-13B, 14A-14B, 15 and 16.

Additionally, the 3D microwave integrated quantum circuit 400M includes, for each bottom/top cap wafer 430, a first electrically conducting layer 450 that covers at least a portion of each of the recesses 420 of the bottom/top cap wafer, and a second electrically conducting layer 350 that covers at least a portion of each of the recesses 320 of the bottom/top cap wafer. During operation of the 3D microwave integrated quantum circuit 400M, all electrically conducting layers 350 and 450 are grounded. In some implementations, either or both of the electrically conducting layers 350, 450 may include a multi-layer material stack, such as, for example, the multi-layer material stacks 2811, 2821 described below with respect to FIG. 28.

Moreover, each recess 420 and each recess 320 of the bottom or top cap wafer 430 is configured to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below an associated cutoff frequency f_(C)−j (i.e., f<f_(C)−j), where the associated cutoff frequency f_(C)−j is larger than an operating frequency f₀−j (i.e., f₀−j<f_(C)−j) of a corresponding quantum circuit device 240-j. For example, a recess 420 of bottom or top cap wafer 430 corresponding to quantum circuit device QC2 is configured to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below cutoff frequency f_(C2) (i.e., f<f_(C2)), where the cutoff frequency f_(C2) is larger than an operating frequency foe (i.e., f₀₂<f_(C2)) of quantum circuit device QC2, while a recess 320 of the bottom or top cap wafer 430 corresponding to quantum circuit device QC5 is configured to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below cutoff frequency f_(CS) (i.e., f<f_(CS)) where the cutoff frequency f_(CS) is larger than an operating frequency f_(0S) (i.e., f_(0S)<f_(CS)) of quantum circuit device QC5. In the latter example, the recess 420 can have a different size in the x-y plane from the recess 320.

As noted above in connection with FIG. 2B, another approach to isolate quantum circuit devices 240 of a microwave integrated quantum circuit uses electrically conducting thru vias. Microwave integrated quantum circuits designed based on this approach are described next.

FIG. 5A is a side view of a 2D microwave integrated quantum circuit 500, and FIG. 5B is a top view of the same circuit in the vicinity of one of a plurality of quantum circuit devices 240 included in the 2D microwave integrated quantum circuit. Here, the 2D microwave integrated quantum circuit 300 includes a first substrate 210, also referred to as a circuit wafer, such that the quantum circuit devices 240 are disposed on a first surface of the circuit wafer 210. Each quantum circuit device QC-j 240, where j=1, 2, 3, . . . , has an associated operating frequency f₀−j. In some implementations, the operating frequencies of the quantum circuit devices 240 are different from each other. In other implementations, at least some of the quantum circuit devices 240 have common operating frequencies.

The 2D microwave integrated quantum circuit 500 further includes electrically conducting vias 560 each extending through the circuit wafer 210 outside of a footprint of each quantum circuit device 240. A length of the electrically conducting vias 560 along the z-axis corresponds to a thickness of the circuit layer 210, which can range from 1 μm to 2 mm. Note that the electrically conducting vias 560 include a material (e.g., Al, In, Ti, Pn, Sn, etc.) that is superconducting at an operating temperature of the 2D microwave integrated quantum circuit 500. In this manner, the 2D microwave integrated quantum circuit 500 can be operated at cryogenic temperatures (e.g., using liquid helium) and the electrically conducting vias 560 (or at least portions thereof) can operate as superconducting vias at that temperature. In addition, during operation of the 2D microwave integrated quantum circuit 500, the electrically conducting vias 560 are grounded.

Moreover, the electrically conducting vias 560 are distributed around the footprint of each quantum circuit device 240 to suppress propagation of electromagnetic waves (also referred to as substrate modes) that have frequencies “f” below a cutoff frequency f_(C) (i.e., f<f_(C)). Such suppression occurs across a volume of the circuit wafer 210 that is adjacent to the footprint of the quantum circuit device. Here, the cutoff frequency f_(C) is larger than the operating frequency f₀ (i.e., f₀<f_(C)) of the surrounded quantum circuit device. The noted suppression of the propagation of the substrate modes is illustrated in FIG. 5A by the relative appearance of an in-air electric field spatial distribution E_(air) and an in-substrate electric field spatial distribution E_(sub) of operating signals.

In this manner, a separation S between adjacent electrically conducting vias 560 is smaller than a maximum separation S_(MAX) corresponding to the cutoff frequency f_(C). In general, structures with parallel metal plates support the propagation of parallel-plate or substrate modes. A resonant frequency of these modes depends on the metal plate area: it drops as the area increases. FIG. 5C is a plot 501 that shows a dependence of the resonant frequency of the first fundamental mode of a square cavity of silicon versus size. Silicon represents one material from which the circuit wafer 210 can be made. Without being limited by theory or mode of operation, the dependence of the resonant frequency may follow the relationship below:

$\begin{matrix} {f_{q} = {\frac{c}{2\pi\sqrt{\epsilon_{r}}}\sqrt{\left( \frac{\pi}{p} \right)^{2} + \left( \frac{\pi}{q} \right)^{2} + \left( \frac{\pi}{r} \right)^{2}}}} & (6) \end{matrix}$

where c is the speed of light in free space, ϵ_(r) is the relative dielectric constant of silicon, and p, q and r are the dimensions of the cavity. Such substrate modes can cause undesired coupling among the quantum circuit devices 240 of the 2D microwave integrated quantum circuit 500, giving rise to a degraded performance of the quantum circuit devices 240. Therefore, if substrate modes have frequencies in a bandwidth that includes the operating frequency of the quantum circuit devices 240, the electrically conducting vias 560 may be used to suppress them.

Referring again to FIG. 5B, a distance DV between the outer perimeter of the surrounded quantum circuit device 240 and a nearest electrically conducting via 560 corresponds to a value of a capacitance between the surrounded quantum circuit device and the nearest electrically conducting via. Moreover, adjacent quantum circuit devices 240 disposed on the circuit wafer 210 can be coupled electromagnetically through a coupling line that includes an electrical conductor 241 extending along the first surface of the circuit wafer over at least a portion of the distance between the adjacent quantum circuit devices. The coupling between the adjacent quantum circuit devices 240 can be capacitive, inductive, or galvanic. In some implementations, one or more electrically conducting vias 560 can be distributed along at least a portion of the coupling line to isolate it from interaction to unwanted modes (e.g., environmental modes), as shown in FIG. 7A.

It was noted above in connection with FIG. 2B that yet another approach to isolate quantum circuit devices 240 of a microwave integrated quantum circuit combines the isolation approach that uses cap wafers, as described relation to FIGS. 3-4, with the isolation approach that uses electrically conducting thru vias, as described in relation to FIG. 5. The design of microwave integrated quantum circuits based on this combined approach are described next.

FIG. 6A is a side view of a 2D microwave integrated quantum circuit 600A that includes electrically conducting vias 560, each extending through the circuit wafer 210 as described in relation to FIGS. 5A-5B. The electrically-conducting vias 560 are in addition to the components of the 2D microwave integrated quantum circuit 300 described in relation to FIGS. 3A-3B. Here, the electrically conducting vias 560 are disposed outside of a footprint of each recess 320 encapsulating an associated quantum circuit device 240. FIG. 6B is a side view of a 2D microwave integrated quantum circuit 600B that includes electrically conducting vias 560, each extending through the circuit wafer 210 as described in relation to FIGS. 5A-5B. The electrically conducting vias 560 are in addition to the components of the 2D microwave integrated quantum circuit 400 described in relation FIG. 4A. Here, the electrically conducting vias 560 are disposed outside of a common footprint of each recess 320 encapsulating an associated quantum circuit device, and respective recess 420 on the other side of the circuit wafer from the encapsulated quantum circuit device. FIG. 6C is a top view of either the 2D microwave integrated quantum circuit 600A or the 2D microwave integrated quantum circuit 600B in the vicinity of one of a plurality of quantum circuit devices 240 included therein.

During operation of the 2D microwave integrated quantum circuit 600A, the electrically conducting layer 350 and the electrically conducting vias 560 are grounded. During operation of the 2D microwave integrated quantum circuit 600B, the electrically conducting layers 350 and 450, and the electrically conducting vias 560 are grounded.

Note that each recess 320 of the cap wafer 310 is configured to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below a cutoff frequency f_(C), where the cutoff frequency f_(C) has been established based on the separation S of the electrically conducting vias 560, as described in relation to FIGS. 5A-5B. The noted suppression of the propagation of the recess modes and of the substrate modes is illustrated in FIG. 6 by the relative appearance of the in-air electric field spatial distribution (i.e., ϵ_(air)) and in-substrate electric field spatial distribution (i.e., ϵ_(sub)) of operating signals. Moreover, (i) the separation S of the electrically conducting vias 560 distributed around the footprint of each recess 320 encapsulating an associated quantum circuit device 240, and (ii) the size WW of the recess are both determined by the cutoff frequency f_(C). As noted above, in the case of the 2D microwave integrated quantum circuit 600A, a separation DV between the perimeter of the quantum circuit device 240 and nearest electrically conducting vias 560 is larger than or at most equal to a separation DW between the perimeter of the quantum circuit device 240 and adjacent walls of the recess 320 of the cap wafer 310.

Moreover, adjacent quantum circuit devices 240 disposed on the circuit wafer 210 can be coupled electromagnetically through a coupling line that includes an electrical conductor 241 extending along the first surface of the circuit wafer over at least a portion of the distance between the adjacent quantum circuit devices. The coupling between the adjacent quantum circuit devices 240 can be capacitive or direct. Note that, as illustrated in FIG. 6C, at least a portion of the coupling line is electromagnetically isolated from environmental noise because it is encapsulated by a trench 321 of the cap wafer 310 and flanked by electrically conducting vias 560 disposed outside the trench.

Referring again to FIG. 6B, the 2D microwave integrated quantum circuit 600B further includes a routing wafer 610. Some electrically conducting lines 650 of the routing wafer 610 are coupled with signal vias 660 extending through the cap wafer 310 to supply control signals to, or retrieve readout signals from, the quantum circuit devices 240 encapsulated in respective recesses 320. The foregoing input-output (I/O) signals can be provided/retrieved through the routing wafer 610 directly from the signal delivery system 106 of the quantum computing system 100 or from quantum circuit devices in adjacent 2D microwave integrated quantum circuit 600B that is stacked vertically, e.g., along the z-axis, as shown below in FIG. 6F. Other electrically conducting lines 650 of the routing wafer 610 are coupled with ground vias 560 extending through the cap wafer 310 to provide ground to the electrically conducting layer 350 (or to the electrically conducting layer 450, or the electrically conducting vias 560 that extend through the circuit wafer 210.)

In the example illustrated in FIG. 6B, the cap wafer 310 has hollow thru vias or apertures 330 into the recess 320. A capacitive coupling can be formed, through such an aperture 330, between a quantum circuit device 240 encapsulated in a recess 320 and an I/O signal carrying electrically conducting line 650.

FIG. 6D is a top view of either the 2D microwave integrated quantum circuit 600A or the 2D microwave integrated quantum circuit 600B. Here, it is shown that the 2D microwave integrated quantum circuit 600A/600B can be scaled to a large number of quantum circuit devices 240 that include multiple qubits 144, resonators 146, 148, tunable couplers 142, and so forth. Here, distances between adjacent qubits 144 can range from 0.5 mm to 5 mm, for instance. Note that recesses 320 of the (top) cap wafer 310 enclose each quantum circuit device 240 formed on the circuit wafer and trenches 321 (which are recesses with a large aspect ratio) of the (top) cap wafer enclose the coupling lines 241. Further note that in the case of the 2D microwave integrated quantum circuit 600B, the contours representing the recess walls can be the common footprint of the recesses 320 of the top cap wafer 310 and the recesses 420 of the bottom cap wafer 410.

Furthermore, a plurality of electrically conducting vias that includes ground vias 560 and I/O signal delivery vias 660 (or other types of via electrically conducting vias that will be described below in connection with FIGS. 7A-7D) are distributed outside of the footprint of the recesses 320 for the 2D microwave integrated quantum circuit 600A, or the common footprint of the recesses 320/420 for the 2D microwave integrated quantum circuit 600B, and between the qubits 144, resonators 146, 148, tunable couplers 142 of the circuit wafer 312. For example, the electrically conducting vias 560 adjacent to the footprint of the recesses 320/420 are grounded, while the electrically conducting vias 660 further apart from the footprint of the recesses 320/420 can be vias 660 that carry signals.

Note that at least some of the electrically-conducting vias 560, e.g., the ones that are far from the footprint of the recesses 320/420, are used mainly to provide thermalization, e.g., because these electrically-conducting vias serve as a heat sink that reduces heat dissipation to the circuit wafer 210. In this manner, the quantum circuit devices 240 disposed on the thermalized circuit wafer 210 can experience reduced loss.

FIG. 6E is a side view of a 3D microwave integrated quantum circuit 600AM that includes multiple 2D microwave integrated quantum circuits similar to the microwave integrated quantum circuit 600A. The outermost layers of the 3D microwave integrated quantum circuit 600AM are the cap wafer 310 and the circuit wafer 210 that have been described in relation to FIG. 3A. Further, the 3D microwave integrated quantum circuit 600AM includes one or more substrates 260 stacked along the z-axis between the cap wafer 310 and the circuit wafer 210, each of the substrates supporting quantum circuit devices 240 included in the 3D microwave integrated quantum circuit 600AM. Note that the substrates 260 are of a different type than the circuit wafer 210 and are referred to as circuit/cap wafers 260. Each circuit/cap wafer 260 has a first surface onto which associated quantum circuit devices 240 are disposed, and a second, opposing surface that defines recesses 320 the correspond to quantum circuit devices 240 disposed on another circuit/cap wafer or circuit wafer 210 adjacent to the second surface of the circuit/cap wafer. Note that the circuit/cap wafer 260 is bonded to each of two adjacent wafers from among a circuit wafer 210, a cap wafer 310, or another circuit/cap wafer, as described in relation to FIGS. 14A-14B, 15 and 16. In addition, spacers (or standoff bumps) may be used between the bonded circuit/cap wafer 260 and each of adjacent wafers, as described below in connection with FIGS. 12, 13A-13B, 14A-14B, 15 and 16.

Additionally, the 3D microwave integrated quantum circuit 600AM includes, for each circuit/cap wafer 260, an electrically-conducting layer 350 that covers at least a portion of each of the recesses 320 of the circuit/cap wafer. Further, for each circuit/cap wafer 260 and for the circuit wafer 210, the 3D microwave integrated quantum circuit 600AM includes electrically conducting vias 560 each extending through the circuit/cap wafer and through the circuit wafer. Here, the electrically conducting vias 560 are disposed outside of a footprint of each recess 320 encapsulating an associated quantum circuit device 240. During operation of the 3D microwave integrated quantum circuit 600AM, all electrically conducting layers 350 and all the electrically conducting vias 560 are grounded.

Note that each recess 320 of the cap wafer 310 and of each of the circuit/cap wafers 260 is configured to suppress propagation inside the recess of electromagnetic waves that have frequencies “f” below an associated cutoff frequency f_(C)−j (i.e., f<f_(C)−j), where the associated cutoff frequency f_(C)−j is larger than an operating frequency f₀−j of a corresponding encapsulated quantum circuit device 240-j (i.e., f₀−j<f_(C)−j). Moreover, the cutoff frequency f_(C)−j has been established based on a separation S-j of the electrically conducting vias 560 distributed around the footprint of recess 320-j encapsulating the associated quantum circuit device 240-j, as described above in connection with FIGS. 5A-5B.

For example, a recess 320-2 of cap wafer 310 corresponding to quantum circuit device QC2 has a width W2 and electrically conducting vias 560-2 extending through the circuit/cap wafer 260 and surrounding the footprint of recess 320-2 are separated by a separation S2 to suppress propagation inside the recess 320-2 of electromagnetic waves that have frequencies “f” below cutoff frequency f_(C2) (i.e., f<f_(C2)), where the cutoff frequency f_(C2) is larger than an operating frequency foe of quantum circuit device QC2 (i.e., f₀₂<f_(C2)); further, a recess 320-5 of the circuit/cap wafer 260 corresponding to quantum circuit device QC5 has a width W5 and electrically conducting vias 560-6 extending through the circuit wafer 210 and surrounding the footprint of recess 320-5 are separated by a separation S5 to suppress propagation inside the recess 320-5 of electromagnetic waves that have frequencies “f” below cutoff frequency f_(CS) (i.e., f<f_(CS)), where the cutoff frequency f_(CS) is larger than an operating frequency f_(0S) of quantum circuit device QC5 (i.e., f_(0S)<f_(CS)). In this example, the width W2 of the recess 320-2 of cap wafer 310 can be different from the width W2 of the recess 320-5 of circuit/cap wafer 260, and the separation S2 of the electrically conducting vias 560-2 extending through the circuit/cap wafer 260 and surrounding the footprint of recess 320-2 can be different from the separation S5 of the electrically conducting vias 560-5 extending through the circuit wafer 210 and surrounding the footprint of recess 320-5.

FIG. 6F is a side view of a 3D microwave integrated quantum circuit 600BM that includes multiple 2D microwave integrated quantum circuits like the microwave integrated quantum circuit 600B stacked along the z-axis. Note that, as each microwave integrated quantum circuit 600B(j), where j=2, . . . , N, includes a routing wafer 610, adjacent microwave integrated quantum circuit 600B(j), 600B(j+1) interface through such a routing wafer. As such, the quantum circuit devices 240 from adjacent microwave integrated quantum circuits 600B(j), 600B(j+1) can be coupled through the routing wafer 610 disposed between them, e.g., in the example shown in FIG. 6F through the routing wafer 610 of the microwave integrated quantum circuit 600B(j+1). For example, the quantum circuit devices 240 from adjacent microwave integrated quantum circuits 600B(j), 600B(j+1) can be capacitively coupled through an aperture 330 in the cap wafer 310 of the microwave integrated quantum circuit 600B(j+1). As another example, the quantum circuit devices 240 from adjacent microwave integrated quantum circuits 600B(j), 600B(j+1) can be directly coupled through a I/O signal carrying via 660 extending through the cap wafer 310 of the microwave integrated quantum circuit 600B(j+1).

Various types of electrically conductive vias will be described next in more detail. Prior to that, note that in addition to the quantum circuit devices 240 disposed on one of the surfaces (e.g., the top surface) of the circuit wafer 210 of at least some of the microwave integrated quantum circuits described above, additional electrically-conducting circuits can be disposed on the opposing surface (e.g., the bottom surface) of the circuit wafer, in some implementations.

FIG. 7A is a top view of a portion of the 3D microwave integrated quantum circuit 600A, for instance. Note that adjacent qubit circuit devices 144 are coupled with each other through a coupler circuit device 142, where the qubit circuit devices and the coupler circuit device are disposed on a circuit/cap wafer 260. Signal vias 660 extending through the circuit/cap wafer 260 provide control signals to and retrieve readout signals from a control/readout resonator disposed on another circuit/cap wafer or circuit wafer 210 (not shown). Coupling lines 241, which can be capacitive, inductive, or direct, are used to in-plane couple the qubit circuit devices 144 with the coupler circuit device 142 and with the signal vias 660.

Note that recesses 320 of the cap wafer 310 or of another circuit/cap wafer 260 encapsulate each of the qubit circuit devices 144 and coupler circuit device 142, while trenches 321 (which are recesses with a large aspect ratio) of the cap wafer 310 or of the other circuit/cap wafer enclose the coupling lines 241. Also note that electrically conducting vias 560 extending through the circuit/cap wafer 260 flank the walls of the recesses 320 and trenches 321. Electrically conducting vias 560 are spaced apart from each other by a separation S related to a cutoff frequency f_(C) associated with operating frequencies f₀ of the qubit circuit devices 144 and coupler circuit device 142, as described in relation to FIGS. 5A-5B. In this manner, the electrically conducting vias 560 are grounded during operation of the 3D microwave integrated quantum circuit 600A to isolate, from spurious substrate modes, the qubit circuit devices 144 and coupler circuit device 142 encapsulated by the recesses 320 and the coupling lines 321 encapsulated by the trenches 321.

FIG. 7B is a close-up perspective view of two quantum circuit devices 240 of the 3D microwave integrated quantum circuit 600A, for instance. A first quantum circuit device 240, a first coupling line 241 and a first contact pad 762 are disposed on the circuit/cap wafer 260 and are encapsulated by a recess 320 of the cap wafer 310. A second quantum circuit device 240, a second coupling line 241 and a second contact pad 762 are displaced along the z-axis from the first quantum circuit device 240, the first coupling line 241 and the first contact pad 762, are disposed on the circuit wafer 210, and are encapsulated by a recess 320 of the circuit/cap wafer 260. Note that in this example, capacitive coupling is established between the first coupling line 241 and the first contact pad 762, and between the second coupling line 241 and the second contact pad 762. However, a direct contact via 662 extending through the recess 320 and remaining thickness of the circuit/cap wafer 260 provides direct contact between the first contact pad 762 and the second contact pad 762.

In the example illustrated in FIG. 7B, the vertical distance between the layers of the 3D microwave integrated quantum circuit 600A is usually set by fabrication technology and flexibility in designing a desired coupling capacitance between quantum circuit devices 240 might be limited if the capacitance is to be made between layers, e.g., along the z-axis. Here, the direct contact via 662 helps with transferring a control signal or a readout signal between layers of the 3D microwave integrated quantum circuit 600A, because a planar coupling capacitance could be designed in a more straightforward manner with much more flexibility.

FIG. 7C is a (x-y) cross-section of a circuit wafer 310 or a circuit/cap wafer 260 in the vicinity of a signal via 660 extending through the circuit wafer or the circuit/cap wafer to transfer control signals or readout signals between the sides of the circuit wafer or the circuit/cap wafer. Note that the signal via 660 is surrounded by electrically conductive vias 560 that are separated from each other by a spacing S. The spacing S is related to a cutoff frequency f_(C) that is larger than operating frequencies f₀ of the signals transferred through the signal via 660. The electrically conductive vias 560 are grounded when signals are being transferred through the signal via 660 to isolate the transferred signals from spurious substrate modes. A radius R of the path of electrically conductive vias 560 surrounding the signal via 660 is related to a capacitance of the arrangement illustrated in FIG. 7C.

FIG. 7D is a (x-y) cross-section of a circuit wafer 310 or a circuit/cap wafer 260 in the vicinity of a DC pad 764. A plurality of direct contact vias 662 extend through the circuit wafer or the circuit/cap wafer to deliver, to the DC pad 764, DC signals from a DC signal source disposed on the opposite side of the circuit wafer or the circuit/cap wafer relative to the DC pad. A DC resistance of the DC connection illustrated in FIG. 7D decreases when the number of direct contact vias 662 increases.

Note that the electrically-conductive vias described in relation to FIGS. 5, 6 and 7—regardless of their function—are formed from a material (e.g., Al, In, Ti, Pn, Sn, etc.) that is superconducting at an operating temperature of the disclosed microwave integrated quantum circuits. Such a material is referred to as a superconducting material. In this manner, the disclosed microwave integrated quantum circuits can be operated at cryogenic temperatures (e.g., using liquid helium) and the electrically-conducting vias (or at least portions thereof) can operate as superconducting vias at that temperature. In some implementations, each of the disclosed electrically-conductive vias comprises a pair of end caps of the superconducting material, where the end caps are disposed adjacent to the first surface and an opposing surface of the circuit wafer 210 or circuit/cap wafer 260. In some implementations, the disclosed electrically-conductive vias have a hollow structure, e.g., are formed as tubes of superconducting material. In some implementations, the disclosed electrically-conductive vias can be filled with conductive material and coated with a layer of superconducting material. For example, the conductive material (which here means a conductive material that is not superconducting at the operating temperature of the disclosed microwave integrated quantum circuits) can be Au, Cu, Pd, and so forth.

The microwave integrated quantum circuits described in relation to FIGS. 3-6 can be fabricated by forming their respective components, e.g., from among circuit wafers 210, circuit/cap wafers 260, cap wafers 310, 410, bottom/top cap wafers 430, or routing wafers 610, and then by bonding together their respective components. Various techniques are described for fabricating and assembling the components of the disclosed microwave integrated quantum circuits. At least some of the disclosed fabrication techniques satisfy one or more of the following capabilities: (i) deep etching processes of thick wafers are used that are capable to form the recesses 320, 420 of the circuit/cap wafers 260, cap wafers 310, 410, bottom/top cap wafers 430 that have a dimension C_(h) of the order of hundreds of microns; (ii) deposition processes are used that are capable of coating superconducting materials (e.g., Al, In, Ti, Pn, Sn, etc.); and (iii) plating processes are used that are capable of filling with a conductor material via holes that are coated with a superconducting material.

A circuit wafer 210 can include signal delivery circuitry of quantum circuit devices 240, e.g., qubits, couplers, and I/O signals, while a routing wafer 610 can includes couplers and I/O signal paths. Thus, processes for their fabrication can be very similar. An example of such fabrication process can include metal patterning on a substrate, machining via holes and metalizing the via holes. The pattering on the substrate could be through metal etching or lift-off depending on the feature sizes.

FIG. 8 shows an example of a method 800 for fabricating either of circuit wafers 210 or routing wafers 610 based on etching. At 810, a metal layer 852 is deposited on a substrate 816. In some implementations, the substrate can be a high-resistivity silicon wafer. In some implementations, the metal layer includes Al or other material (e.g., In, Ti, Pn, Sn, etc.) that is superconducting at an operating temperature of the disclosed microwave integrated quantum circuits. Here, the Al deposition is performed by either sputtering or e-beam evaporation methods. Note that deposition of a Ti adhesion layer might be needed.

At 820, a photoresist layer 822 is spun on the metal layer 852. Additionally, the photoresist layer 822 can be soft-baked.

At 830, the photoresist layer 822 is patterned for metal features. In some implementations, when higher resolution pattering is required for the circuit wafer 210, this operation is performed using E-beam lithography. In other implementations, the photoresist layer 822 is exposed and developed.

At 840, the metal layer 852 is wet-etched to obtain metal features 650. An etch mask used for the wet etch is the patterned photoresist layer 822.

At 850, the patterned photoresist layer 822 is stripped to expose the metal features 650. Operations 810-850 can be repeated for depositing additional metal layers or a metal oxide (e.g., Al₂O₃). At this point, fabrication of a circuit wafer 210 may be completed. If via holes also are needed in the circuit wafer 210 or a routing wafer 610, the method 800 continues in the following manner:

At 860, another photoresist layer 824 is spun on the metal layer 852 on the circuit wafer 210.

At 870, the photoresist layer 824 is patterned for vias. In this example, the photoresist layer 824 is exposed and developed.

At 880, the substrate 816 is thru etched to obtain a via hole 330. In some implementations, the via hole 330 is obtained through wet-etching. In other implementations, the via hole 330 is obtained through dry etching.

At 890, the patterned photoresist layer 824 is stripped to expose the metal features 650.

In some implementations, operations 860-890 can be replaced with a laser drilling process in the following manner. As a first operation, a protective layer is deposited on sensitive areas of the circuit wafer 210 or routing wafer 610. As a second operation, the via hole 330 is drilled using a laser. At a third operation, the protective layer is removed from the sensitive areas of the circuit wafer 210 or routing wafer 610.

As noted above, the metal features 650 on the substrate 816 could be obtained through a lift-off process as an alternative to operations 810-850. Such lift of process can be performed in the following manner: (i) Photoresist is spun, then soft baked; (ii) Either one of an e-beam lithography with a reverse mask, or alternatively, a photoresist development bake can be used to pattern the photoresist; (iii) Al is deposited over the patterned photoresist by either sputtering or e-beam evaporation methods. Note that deposition of a Ti adhesion layer might be needed; and (iv) The patterned photoresist is stripped for lift-off. In this case, Al is lifted-off from areas of the patterned photoresist.

An alternative method to reduce or avoid the possibility of damaging sensitive superconducting circuit components during laser drilling or etching vias is to perform via drilling/etching process in the first step. Depending on the sizes/dimensions of the vias, spinning a uniform layer of photoresist might not be practical in some instances. One solution is to fill the vias with Al or In (or with any superconducting paste) and polish the surface.

Cap wafers 310, 410, bottom/top cap wafers 430, or circuit/cap wafers 260 can be fabricated from substrates (e.g., wafers) that include one or more of Si, Al₂O₃, SiO₂, Si₃N₄ (or another silicon nitride stoichiometry), SiO_(x), lithographically defined thick photoresists (such as SU8, etc.) or superconducting metals. Processes that used to fabricate either of cap wafers 310, 410, bottom/top cap wafers 430, or circuit/cap wafers 260 include (i) micromachining of recesses 320, 420 and trenches 321, and (ii) deposition of a superconducting material to at least partially cover the walls and bottom of the micromachined recesses and trenches.

Processes for fabricating either of wafers 310, 410, bottom/top cap wafers 430, or circuit/cap wafers 260 from thick Si wafers or silicon-on-insulator (SOI) wafers will be described. TABLE 1 lists processes for fabricating either of cap wafers 310, 410, bottom/top cap wafers 430, or circuit/cap wafers 260 that are described in detail below.

TABLE 1 Process Process Process Process 900 1100 1000 1150 Structural Si SOI SU-8 material Process Wet etch DRIE DRIE or wet SU-8 expose etch & develop Described in 9 11A 10 11B-11C connection with FIG. Photoresist Hard (SiO₂, Soft and thick Soft and N/A Si₂N₄, metals) thick Etch depth Required Required Not required N/A control (timing) (timing) Walls Angled/ Vertical/ Either Vertical/ smooth scalloped smooth Cost Medium Medium High Low

FIG. 9 shows an implementation of a process 900 for fabricating either one of cap wafers 310/410, bottom/top cap wafers 430, or circuit/cap wafers 260 using wet-etching of Si wafers 916. Here, a Si wafer 916 can be up to 2 mm thick.

At 910, a hard mask 912 is deposited on a Si wafer 916. As photoresists do not hold up to wet etchants, the hard mask 912 can be SiO₂, Si₃N₄ (or another silicon nitride stoichiometry) and metals. For example, low pressure chemical vapor deposition (LPCVD) of 1 μm of SiO₂ is performed in a furnace tube, e.g., Tempress TS 6604 S1 (that can be used to deposit low temperature oxide).

At 920, photoresist 922 is spun on the hard mask 912. Then, the photoresist 922 is soft baked. For example, photoresist S1813 can be used to obtain a film of about 1.3 μm thickness. First, photoresist S1813 is dispensed at 900 rpm for 5 seconds, then spun at 4000 rpm for 60 seconds. Then, the spun photoresist is soft baked on a hot plate at 115° C. for 60 seconds.

At 930, the photoresist 922 is exposed, developed and hard baked. In this manner, the lateral dimensions (e.g., a width) WW and locations in the (x-y) plane of recesses 320 are defined at this operation. For example, the soft baked photoresist is exposed with GCA 8500 G-Line (0.35 NA), then developed with MIF-319 developer for 60 seconds. Finally, the developed resist is rinsed with DI water and dried.

Alternative to operations 920 and 930, features of the photoresist 922 can be laser printed.

At 940, the hard mask 912 is etched. Wet or dry etching can be used depending on the material of the hard mask 912. As the hard mask 912 is about 1 μm thick, the wet etch undercut is not a concern given the tolerances. For example, buffered hydrofluoric acid is used (etch rate for LPCVD SiO₂: 120 nm) for 8 minutes and 20 seconds to etch 1 mm of SiO₂. The etched SiO₂ is then rinsed with DI water and dried.

At 950, the Si wafer 916 is wet-etched to form recesses 320 with a depth C_(h). Possible etchants are an aqueous solution of HNO₃+HF, a solution of KOH in isopropyl alcohol, an aqueous solution of ethylene diamine and pyrocatechol (EDP), and an aqueous solution of tetramethylammonium hydroxide (TMAH). The recommended etchant for different materials of the masks 912 are listed in TABLE 2.

TABLE 2 Operating R100 S = R₁₀₀/ Mask material Etchant Temp (° C.) (μm/min) R₁₁₁ SiO₂, Si₃N₄, Au, Ethylenediamine 100 0.47 17 Cr, Ag, Cu pyrocatechol (EDP) SiO₂, Si₃N₄ (etches KOH/isopropyl 50 1.0 400 at 2.8 nm/min) alcohol (IPA) SiO₂, Si₃N₄ Tetrametyl- 80 0.6 37 ammonium hydroxide (TMAH)

Note that common Si wet etchants are usually anisotropic with an etch rate depending upon orientation to crystalline planes. For instance, for <100>-oriented wafers, KOH selectively etches the <111> crystallographic plane, which results in angled sidewalls) (54.7°. Etch depth must be time-controlled after characterizing the etch rate for the specific etchants conditions (temperature, etc.). Etching is stopped when a depth equal to a dimension C_(h) of a recess 320 is obtained. For example, a wet process is used based on an available recipe and a desired etch depth. Etch time for a target depth of a recess 320 is calculated based on etch rate. The etched recess 320 is then rinsed with de-ionized (DI) water and dried.

At 960, the patterned photoresist 922 and the hard mask 912 are removed. In this manner, a cap wafer 310 that has recesses 320 with a width WW and a depth C_(h) is obtained. For example, the SiO₂ is removed using HF or BHF. Note that the photoresist 922 may be removed before operation 950, otherwise it lifts off during the wet etching. Finally, the cap wafer 310 is rinsed with DI water and dried.

FIG. 10 shows an implementation of another process 1000 for fabricating either of cap wafers 310/410, bottom/top cap wafers 430, or circuit/cap wafers 260 using wet-etching of Si on insulator (SOI) wafers 1012. In other implementations, a Si-insulator-Si (SIS) wafer can be used, where an insulator layer is sandwiched between two Si layers. An SOI wafer 1012 includes an insulator layer 1114 and a Si layer 1116. The insulator layer 1114 can include one or more of SiO₂, Si₃N₄ (or another silicon nitride stoichiometry), Al₂O₃, etc.

A depth C_(h) of a recess 320 is given by the thickness (e.g., 0.5 mm-1.5 mm) of the Si layer 1016 of the SOI wafer 1012. The thickness of the Si layer 1016 is measured between the outer surface 1024 of the SOI wafer 1012 and the interface 1018 between the Si layer and the insulator layer 1014. In the example illustrated in FIG. 10, the insulator layer 1014 of the SOI wafer 1012 is used as an etch stop to avoid difficulties associated with characterization of etch rates. As the insulator layer 1014 has high selectivity to Si etchants, time-controlled etching is not required for process 1000.

At 1010, a hard mask 912 is deposited on the Si layer 1016. For example, LPCVD of 1 μm of SiO₂ is performed in a furnace tube, e.g., Tempress TS 6604 S1 (that can be used to deposit low temperature oxide).

At 1020, the hard mask 912 is patterned to define the lateral dimensions (e.g., a width) WW and locations in the (x,y) plane of the recess 320. For example, photoresist S1813 can be used to obtain a film of about 1.3 μm thickness. First, photoresist S1813 is dispensed at 900 rpm for 5 seconds, then spun at 4000 rpm for 60 seconds. The spun photoresist is soft baked on a hot plate at 115° C. for 60 seconds. The soft baked photoresist is exposed with GCA 8500 G-Line (0.35 NA), and developed with MIF-319 developer for 60 seconds. Finally, the developed resist is rinsed with de-ionized water and dried. Then, the SiO₂ hard mask 912 is etched using buffered hydrofluoric acid. The etching of the SiO₂ hard mask 912 may take around 8 minutes and 20 seconds, depending on the etch rate and thickness of the SiO₂ hard mask. Finally, the etched SiO₂ hard mask 912 is rinsed with DI water and dried. Note that the photoresist may be removed before operation 1030, otherwise it lifts off during the wet etching.

At 1030, the Si layer 1016 is wet etched to obtain the recess 320 with a depth Cr, equal to the thickness of the Si layer. One of the wet etch recipes listed in TABLE 2 can be used, although no timing is necessary in this case, as the wet etching of the Si layer 1016 will stop at the interface 1018 between the Si layer and the insulator layer 1014. The etched recess 320 is then rinsed with DI water and dried.

At 1040, the patterned photoresist and the hard mask 912 are removed. In this manner, a cap wafer 310 that has recesses 320 with a width WW and a depth C_(h) is obtained. For example, the SiO₂ hard mask 912 is removed using HF or BHF. Finally, the cap wafer 310 is rinsed with DI water and dried.

FIG. 11A shows an implementation of another process 1100 for fabricating either of cap wafers 310/410, bottom/top cap wafers 430, or circuit/cap wafers 260 using deep reactive-ion etching (DRIE) of Si wafers 916. DRIE is a highly anisotropic etch process used to create deep, steep-sided recesses 320 and trenches 321 in Si wafers 916, with aspect ratios of 20:1 or more. Here, a Si wafer 916 can be up to 2 mm thick.

At 1110, a mask layer 1122 is deposited on the Si wafer 916. In some implementations, the mask layer 1122 is a layer of thick photoresist that is spun onto the Si wafer 916, and then soft baked. In other implementations, the mask layer 1122 j can be a layer of SiO₂ or Si₃N₄ (or another silicon nitride stoichiometry) which have high selectivity to Si etchants. Note that metal masks are not desirable as they sputter inside the DRIE chamber and result in high surface roughness. For example, a 24 μm thick film of AZ 9260 photoresist can be deposited on the Si wafer 916 in the following manner: (i) first coat target: 10 μm film thickness: dispense: static or dynamic @ 300 rpm spin: 2400 rpm, 60 seconds; (ii) edge bead removal rinse: 500 rpm, 10 second dry: 1000 rpm, 10 sec; (iii) first soft bake 110° C., 80 second hotplate; (iv) second coat target: 24 μm total film thickness: dispense: static or dynamic @ 300 rpm spin: 2100 rpm, 60 seconds; (v) edge bead removal rinse: 500 rpm, 10 second dry: 1000 rpm, 10 second; and (vi) second soft bake 110° C., 160 second hotplate.

At 1120, the mask layer 1122 is patterned to define the lateral dimensions (e.g., a width) WW and the locations in the (x,y) plane of the recess 320. For example, the mask layer 1122 that is a thick photoresist layer is exposed, developed and hard baked. Here, the 24 μm thick film of soft baked AZ 9260 photoresist is patterned in the following manner: (i) exposure dose (10% bias) 2100 mJ/cm², broadband stepper; (ii) development AZ® 400K Developer 1:4, 260 second spray dispense temp. 27° C. rinse: 300 rpm, 20 second dry: 4000 rpm, 15 seconds; and (iii) rinse with de-ionized water and dry.

As another example, if the mask layer 1122 is a layer of SiO₂ or Si₃N₄ (or another silicon nitride stoichiometry), then photolithography operations described above in connection with FIGS. 9 and 10 are used to pattern the layer of SiO₂ or Si₃N₄. Moreover, laser printing can be used as an alternative method to operations 1110 and 1120.

At 1130, the Si layer 1016 is etched using DRIE to obtain the recess 320 with a depth C_(h). For example, a Bosch DRIE process can be used. This process contains successive cycles of etching and passivation with the flow of SF₆ and C₄F₈ gases. C₄F₈ source gas yields a substance similar to Teflon. Scalloped etched walls are common features of DRIE which could be made smooth by lowering the etch rate. Etch depth (e.g., for obtaining the target depth C_(h)) must be time-controlled after characterizing the etch rate for specific chamber conditions (temperature, pressure, gas content, etc.).

At 1140, the patterned photoresist mask layer 912 is removed. In this manner, a cap wafer 310 that has recesses 320 with a width WW and a depth C_(h) is obtained. For example, the 24 μm thick film of hard baked AZ 9260 photoresist is stripped in the following manner: wet photoresist stripper (NMP: 1-Methyl-2-pyrrolidon or DMSO: dimethyl sulfoxide) or dry oxygen plasma. For 20+ μm photoresist film thickness about 15 minutes is sufficient to remove it all. Then, the cap wafer 310 is rinsed with DI water and dried.

FIG. 11B shows an implementation of another process 1150 that uses SU-8 as structural material for fabricating either of cap wafers 310/410, bottom/top cap wafers 430, or circuit/cap wafers 260. SU-8 is an epoxy-based, highly viscous, negative photoresist. It can be spun up to a thickness above 1 mm (normally with multiple spinning steps) and still be processed with optical contact lithography methods. SU-8 has been used to fabricate high aspect ratio waveguide structures. By using SU-8, the bulk micromachining process can be performed through exposure and developing the photoresist rather than etching silicon. As a result, the sidewalls of the recesses 320 are vertical and smooth. In general, cap wafers 310 do not need to have any specific conditions (thickness, crystal planes, etc.) as it remains intact and serves only as the holder during the process.

At 1160, an SU-8 layer 1152 is spun on a substrate 1116. The substrate 1116 can be a Si wafer, an insulator wafer, a ceramic wafer or a metallic plate. Here, a thickness of the SU-8 layer 1152 can be equal to or larger than the depth C_(h) of the recess 320. The spun SU-8 layer 1152 is then baked. FIG. 11C is a plot 1101 that shows dependence of film thickness on the spin speed, for two SU-8 materials.

Referring again to FIG. 11B, at 1170, the baked SU-8 layer 1152 is patterned to obtain a recess with lateral dimensions (e.g., a width) WW at a desired location in the (x,y) plane. Here, the baked SU-8 layer 1152 is first exposed and then developed. A total processing time of operations 1160 and 1170 can take about 10 min.

After the cap wafers 310/410, bottom/top cap wafers 430, or circuit/cap wafers 260 have been fabricated using either of the fabrication processes 900, 1000, 1100 or 1150, at least portions of the cap wafers, bottom/top cap wafers, or circuit/cap wafers that include the recesses 320/420 and trenches 321 are coated with an electrically conducting layer that is superconducting at operating temperatures of quantum computing systems 100. In some implementations, spacers (also referred to as standoff bumps) are formed, on a surface of the cap wafers, bottom/top cap wafers, or circuit/cap wafers, between recesses 320/420 and trenches 321, prior to depositing the electrically conducting layer. The standoff bumps are used to control (i) a spacing between a cap wafer on which they are formed with another wafer to which the cap wafer is bonded, and (ii) forces applied, during the bonding process, to a bonding line between the bonded wafers. In some implementations, indium bumps are deposited on a surface of the cap wafers, bottom/top cap wafers, or circuit/cap wafers, between recesses 320/420 and trenches 321, after depositing the electrically conducting layer. The indium bumps are used to bond a cap wafer on which they are formed with another wafer to which the cap wafer is bonded. In some implementations, the electrically conducting layer includes a multi-layer material stack. For example, the electrically conducting layer may be similar to stack 2811 or the stack 2821 described below with respect to FIG. 28. In some instances, the electrically conducting layer includes one or more layers of non-superconducting material, but maintains one or more properties of superconductivity (e.g., a zero (0) or near-zero resistance, such as less than one (1) milliohm (mu)).

FIG. 12 shows an implementation of another process 1200 for fabricating cap wafers, for instance, where a fabricated cap wafer 310A has standoff bumps 1215, is coated with an electrically conducting layer 350, and further has In bumps 1284. The process 1200 has four stages: (i) forming the standoff bumps 1215; (ii) forming the recesses 320; (iii) coating the electrically conducting layer 350; and (iv) forming the In bumps 1284.

Stage (i), or forming the standoff bumps 1215, includes the following operations: at 1202, a SiO₂ layer 1214 is thermally grown on a Si wafer 916. A thickness of the SiO₂ layer 1214 defines the height of the standoff bumps 1215.

At 1204, a photoresist layer 1222 is patterned to define the location in the (x-y) plane of the standoff bumps 1215. The patterned photoresist layer 1222 will be used as a mask for etching the SiO₂ layer 1214.

At 1206, the SiO₂ layer 1214 is etched to form the standoff bumps 1215 at their desired location in the (x-y) plane. The photoresist layer 1222 is now stripped and the Si wafer 916 that supports the standoff bumps 1215 is cleaned in preparation for the next stage of process 1200.

Stage (ii), or forming the recesses 320, includes the following operations: at 1220, a photoresist layer 1222 is patterned on the Si wafer 916 to define the lateral dimensions (e.g., a width) WW and the locations in the (x,y) plane of the recesses 320. This operation can be performed in a manner similar to the way operation 1120 of process 1100 is performed.

At 1240, the Si wafer 916 is etched using DRIE, and then the photoresist layer 1222 is removed. In this manner, recesses 320 with a depth C_(h) are obtained. This operation can be performed in a manner similar to the way operation 1130 of process 1100 is performed. The photoresist layer 1222 is now stripped (in a manner similar to the photoresist stripping 1140 of process 1100), and, hence, the Si wafer 916—that supports the standoff bumps 1215 and has the recesses 320—is ready for the next stage of process 1200.

Stage (iii), or coating the electrically conducting layer 350, includes the following operations: at 1250, the electrically conducting layer 350 is coated on the Si wafer 916, over the standoff bumps 1215 and, at least in part, over the recesses 320. For example, a layer of Al having a thickness in the range of 0.1-2 μm is coated using sputter deposition. Sputtering is a non-directional physical vapor deposition (PVD) process which provides the best step/sidewall coverage among all the PVD and chemical vapor deposition (CVD) methods. In this manner, the base and the sidewalls of the recesses 320, and the top and the sidewalls of the standoff bumps 1215 can be effectively covered. To ensure the required thickness on the sidewalls, a layer 350 that is at least twice as much thicker than required is deposited especially for the cases where sidewalls are vertical. After the deposition, EDX could be used to measure the thickness of the deposited layer 350. In some implementations, sub-steps performed at 1250 can be: (a) oxygen plasma treatment to enhance aluminum adhesion; and (b) sputtering aluminum twice as thick as the minimum required thickness to ensure sidewall coverage. Note that a Ti adhesion layer might be needed. In some implementations, a cold/hot deposition can be used for smoother step coverage. The cold/hot deposition consists of cumulatively depositing two layers of Al at different temperatures to achieve a desired total thickness of the electrically conducting layer 350. At this point, the Si wafer 916—that supports standoff bumps 1215, has recesses 320, and is coated with an electrically conducting layer 350—is ready for the next stage of process 1200.

Stage (iv), or forming the indium bumps 1284, includes the following operations: at 1260, a negative photoresist layer 1224 is spun on the electrically conducting layer 350. Here, the negative photoresist layer 1224 is coated in a conformal manner to cover the sidewalls of the recesses 320. For this purpose, the negative photoresist layer 1224 has a thickness of up to 10 μm.

At 1270, the negative photoresist layer 1224 is patterned to define openings 1272 in the negative photoresist layer that correspond to locations in the (x-y) plane of the indium bumps 1284. Note that the indium bumps 1284 are disposed between the recesses 320. Although not shown in FIG. 12, but shown in FIGS. 14A-14B, the indium bumps 1284 can be formed based on a pattern that includes channels used to pump out the trapped gas between bumps. This is advantageous because the disclosed microwave integrated quantum circuits will experience low pressure inside dilution refrigerators, and, therefore, trapped gases should be pumped out.

At 1280, the indium bumps 1284 are formed. Before the forming of the indium bumps 1284, a Ti adhesion layer 1282 is formed on the electrically conducting layer 350 inside the openings 1272. Then, the indium bumps 1284 are evaporated on the Ti adhesion layer 1282, such that a height of the In bumps is larger than a total height of the standoff bumps 1215 coated with the electrically conducting layer 350. Once the patterned negative photoresist layer 1224 has been removed, the cap wafer 310A is ready to be bonded to a circuit wafer 210 as part of any of the microwave integrated quantum circuits described above. Note that the cap wafer 310A formed by using process 1200 has standoff bumps 1215, has recesses 320 of width WW and depth C_(h), is coated with an electrically conducting layer 350, and further includes indium bumps 1284.

As described in relation to FIGS. 5 & 6, electrically conducting vias 560, 660, 662 have an important role in isolating quantum circuit devices 240 from each other and from spurious substrate modes, in reducing thermal noise in microwave integrated quantum circuits, in transferring control signals and readout signals between different quantum circuit devices and/or between the quantum circuit devices and the signal delivery system 106. FIGS. 13A-13B show an example of a process 1200 for fabricating any of the electrically conducting vias 560, 660, 662 extending through any of the cap wafers or circuit wafers described herein.

At 1305, a Si wafer 916 is etched using DRIE to form via holes 330 (or openings having a high aspect ratio of 20:1 or more, i.e., openings that are deep and narrow, with steep sidewalls. Operation 1305 includes sub-operations that can be performed in a manner similar to the way the operations 860-890 of process 800 are performed, or to the way the operations of process 1100 are performed.

At 1310, a metal layer 1312—that is superconducting at an operating temperature of the quantum processor cell 102—is deposited. Here, a barrier layer 1311, made from Si₃N₄ (or another silicon nitride stoichiometry), is formed using low pressure chemical vapor deposition (LPCVD). In this manner, the barrier layer 1311 is formed on the Si wafer 916 to coat the via holes 330. Ti is a superconductor with a critical temperature of 300 mK, and, hence, Ti is a metal that is superconducting at the operating temperature (T_(op)<300 mK) of the quantum processor cell 102. In this manner, the metal layer 1312, made from Ti using LPCVD, is formed on the barrier layer 1311 to coat the via holes 330. As the via holes 330 that are lined with the Si₃N₄ layer 1311 and the Ti layer 1312 will be filled with Cu as part of an upcoming operation of process 1300, a Cu seed layer 1313 is formed next on the Ti layer. Here, the Cu seed layer 1313 is formed using metal-organic chemical vapor phase deposition (MOCVD).

At 1315, a Cu layer 1314 is plated over the Cu seed layer 1313 and fills the inside of the via holes 330 to form blind vias 1316. Here, the plating recipe is adjusted to prevent void creation inside the via holes 330. Further here, the Si₃N₄ layer 1311 and Ti layer 1312 are used to prevent the diffusion of Cu from inside the blind via 1316 to the Si wafer 916.

At 1320, layers are removed from the top of the Si wafer 916. First, the overburden Cu layer 1314 is removed using chemical mechanical polishing (CMP). The first CMP is stopped on the Ti layer 1312. A post CMP cleaning is performed next, followed by annealing at 400° C. for 1 h or 300° C. for 2 h (to release wafer tension). Second, the Ti layer 1312 and then the Si₃N₄ layer 1311 are removed using CMP. Here, an additional layer of thickness 0.5 μm from the Si wafer 916 is CMP-ed to remove the contamination diffused on the surface of the Si wafer. A surface 1306 of the Si wafer 916 is formed in this manner.

At 1325, the blind vias 1316 are capped with Ti caps 762 to form single-capped vias 1326. First, a layer of Ti is formed on the surface 1306 of the Si wafer 916 over the blind vias 1316; photoresist is spun on the layer of Ti is patterned to define the size of the caps 762; then the layer of Ti is wet etched to form the Ti caps 762; also, Ti oxide is cleaned from the Ti caps 762 using reverse sputtering (here, reverse sputtering is a process where an Ar plasma is run with no target, therefore, instead of deposition of material from the target, etching from the substrate happens and the oxide layers on the Ti caps are etched away). Second, an Al layer 1328 is formed on the surface 1306 of the Si wafer 916 over the single-capped vias 1326; photoresist spun on the Al layer 1328 is patterned to define desired Al features (e.g., coupling line, signal lines, etc.); then the Al layer 1328 is wet etched to form the desired Al features.

At 1330, a passivation layer 1332 is formed on the surface 1306 of the Si wafer 916. The passivation layer 1332 is chosen to be resistant to the developing and etching chemistries which happen at later stages and to be robust at cryogenic temperatures. For instance, the passivation layer 1332 can be a polyimide, e.g., PBO (Polybenzoxazoles) or BCB (Benzocyclobutene). The passivation layer 1332 is patterned to define openings 1334 over at least some of the single-capped vias 1326 and the features of the Al layer 1328.

At 1335, an under-bump metal layer 1336 inside the openings 1334 of the passivation layer 1332 is formed. In this manner, the under-bump metal layer 1336 is formed on the Ti caps 762 of the single-capped vias 1326 and on the features of the Al layer 1328. The under-bump metal layer 1336 can be formed from Ti/Pd or Ti/Pt using sputter deposition. The goal of operation 1335 is to deposit a metal which is solderable on surfaces of metals that are not solderable. For example, Al is not solderable, so bonding to the features of the Al layer 1328 would be challenging if the under-bump metal layer 1336 were not deposited.

At 1340, a temporary carrier 1342 is bonded to the passivation layer 1332. As the Si wafer 916 will be thinned down during an upcoming operation of process 1300, the carrier wafer 1342 will ease future handling of the Si wafer.

At 1345, the Si wafer 916 is thinned down until ends of the single-capped vias 1326 are revealed and a surface 1346 is formed. As the thinning down is performed using CMP, the resulting surface 1346 of the Si wafer 916 can be smooth.

At 1350, the single-capped vias 1326 are capped at their respective revealed ends with Ti caps 762 to form double-capped vias 1352, referred to simply as capped vias 1352. First, CuO is removed from the revealed ends of the single-capped vias 1326 using reverse sputtering. Second, another layer of Ti is formed on the surface 1346 of the Si wafer 916 over the capped vias 1352; photoresist spun on the other layer of Ti is patterned to define the size of the caps 762; then the other layer of Ti is wet-etched to form the Ti caps 762 on the surface 1346 of the Si wafer 916. Here, the surface 1346 is cleaned with Acetone (ultrasonic bath), isopropyl alcohol (ultrasonic bath), dehydration (i.e., vacuum or an N2 gas environment for 1 hour), and exposure to an O₂ plasma. In this manner, the capped vias 1352 include bulk Cu (which is an electrical conductor but is non-superconducting at operating temperatures) capped with and surrounded by Ti (which is superconducting at operating temperatures). In this manner, the non-superconducting material inside the capped vias 1352 will not be exposed to electromagnetic fields in the Si wafer 916.

At 1355, a negative photoresist layer 1224 is formed on the surface 1346 of the Si wafer 916. The negative photoresist layer 1224 is then patterned to define openings 1356 to the surface 1346.

At 1360, a layer of Ti/Pd is deposited over the patterned negative photoresist layer 1224. The patterned negative photoresist layer 1224 is then lifted-off to form alignment marks 1362 for e-beam writing on the surface 1346 of the Si wafer 916. Here, the surface 1346 of the Si wafer 916 is cleaned.

At 1365, a negative photoresist layer 1224 is formed on the surface 1346 of the Si wafer 916. The negative photoresist layer 1224 is then patterned to define size and location of Al features to be formed on the surface 1346. Ti oxide is removed from the alignment marks 1362 using reverse sputtering.

At 1370, another Al layer 1328 is formed over the patterned negative photoresist layer 1224 to cover the alignment marks 1362. The patterned negative photoresist layer 1224 is then lifted-off to form features of the Al layer 1328 that cover the alignment marks 1362.

At 1375, the carrier wafer 1342 is de-bonded from the passivation layer 1332. In addition, the Si wafer 916 is diced into smaller pieces.

At 1380, the features of the Al layer 1328 that cover the alignment marks 1362 are modified. First, the surface 1346 of the Si wafer 916 is cleaned, then aluminum oxide is removed, then negative photoresist is spun and patterned. Second, a double-angle Al evaporation is performed, followed by lift-off to obtained modified features of the Al layer 1328 that cover the alignment marks 1362.

In this manner, the process 1300 can be used to form pieces of Si wafer 916 and capped vias 1352 extending through the Si wafer from a surface 1306 to the opposing surface 1346. Features of an Al layer 1328 cover alignment marks 1362 formed on the 1346 surface. Another Al layer 1328 has different features on the surface 1306. A passivation layer 1332 is attached to the surface 1306 of the Si wafer 916. An under-bump metal layer 1336 is disposed inside openings of the passivation layer 1332 on Ti caps of at least some of the capped vias 1352 and on at least some of the features of the Al layer 1328 on the surface 1306 of the Si wafer 916.

As described above, the various types of cap wafers (e.g., 310, 410, 430, 260) are bonded together with various types of circuit wafers (e.g., 210, 260) to form 2D microwave integrated quantum circuits (e.g., 300, 400, 500, 600A, 600B) or 3D microwave integrated quantum circuits (e.g., 400M, 600AM, 600BM). The bonding methods described below, that are used to fabricate such microwave integrated quantum circuits, satisfy one or more of the following features. Bonding elements (e.g., bumps, balls, etc.) used by the disclosed bonding processes are superconducting at cryogenic temperatures (˜10 mK) so that the bonding elements do not induce additional loss mechanism to the quantum circuit devices 240, which operate at the cryogenic temperature. Temperature is maintained low (e.g., <100° C., preferably <80° C.) during some of the disclosed bonding processes due to the heat sensitivity of Josephson junctions of some of the quantum circuit devices 240. For example, force-only bonding (at room temperature) is used in some cases. As another example, Al—Al bonding can be performed at low temperatures if the native grown oxide on the surface of Al pads is removed (by plasma surface treatment, for instance). As yet another example, ductile material, e.g., indium, is preferable because its oxide can be broken by applying pressure and deforming it. Bonding interfaces are not hermetic because the disclosed microwave integrated quantum circuits will experience low pressure inside dilution refrigerators, and, therefore, trapped gases should be pumped out.

FIG. 14A shows an example of a process 1400 for fabricating a 2D microwave integrated quantum circuit, e.g., like the 2D microwave integrated quantum circuit 600A described above in connection with FIG. 6A.

At 1410, a circuit wafer 210 and a cap wafer 310A are received. Here, the circuit wafer 210 supports quantum circuit devices 240 (only one of which is shown in FIG. 14A). Note that process 1300 has been used to fabricate electrically conducting thru vias 560 and Al features 1284 of the circuit wafer 210. Moreover, process 1200 has been used to fabricate the cap wafer 310A that has recesses 320 and standoff bumps 1215. FIG. 14A depicts only one such cap wafer. However, this depiction is not intended as limiting. Other numbers of cap wafers are possible. The cap wafer 310A is coated with an electrically conducting layer 350 and has indium bumps 1284 connected to the electrically conducting layer through a Ti adhesion layer 1282.

At 1420, the circuit wafer 210 is cold bonded to the cap wafer 310A. Here, the bonding is performed using a press 1422, in which circuit wafer 210 can be held fixed while applying pressure to the cap wafer 310A against the circuit wafer. The press 1422 can be part of a dedicated mechanical fixture, or part of an integrated bonding system, e.g., a flip-chip bonder. As described in relation to FIG. 12, the height of the indium bumps 1284 before bonding is larger than the total height of the stand-off bumps 1215 coated with the electrically conducting layer 350. Therefore, a value of the pressure experienced by the indium bumps 1284, as they deform when the press 1422 applies pressure to the cap wafer 310A, is controlled by the height of the coated standoff bumps 1215. In fact, the deforming pressure is maximum when an air gap is formed between the cap wafer 310A and the circuit wafer 210 that has a gap thickness equal to the height of the coated standoff bumps 1215. Additionally, the deformed In bumps 1284* are thicker and shorter (e.g., >35% shorter) than the In bumps 1284 before bonding.

In general, bonding two naturally oxidized metallic layers includes removing or breaking the oxides from both sides to create metal-metal bonds. As such, the pressure applied on the cap wafer 310 has to exceed a threshold pressure that allows: (i) breakage of the naturally grown indium oxide (e.g., In₂O₃) to expose barren indium on the deformed In bumps 1284*, and (ii) breakage of the naturally grown Al₂O₃ to expose Al on the Al features 1328, in order to create metal-metal bonds necessary for bonding. To lower the threshold pressure, in some implementations, the receiving operation 1410 includes dispersing sharp, edged diamond nanoparticles 1412 over the indium bumps 1284 so that the indium oxide layer on the deformed indium oxide bumps 1284* and the Al₂O₃ layer on the Al features 1328 can easily be broken when pressure is applied. Note that the bonding operation 1420 is performed at temperatures that do not exceed 100° C., e.g., at temperatures less than 80° C.

A process 1400M for fabricating a 3D microwave integrated quantum circuit, e.g., like the 3D microwave integrated quantum circuit 600A described above in connection with FIG. 6E is described next. The process 1400M includes performing the operation 1410 of the process 1400, and performing an appropriate number of iterations of the operation 1420 of process 1400.

At 1410M, a circuit wafer 210 and a cap wafer 310A are received as described in connection with the operation 1410 of the process 1400. In addition, at 1410M, N circuit/cap wafers 260A are received, as illustrated in FIG. 14B. Here, the circuit wafer 210 and the circuit/cap wafers 260A each supports quantum circuit devices 240 (only one of which is shown in FIG. 14B). Note that the process 1300 has been used to fabricate electrically conducting thru vias 560 and Al features 1284 of the circuit wafer 210 and of the circuit/cap wafers 260A. Moreover, process 1200 has been used to fabricate the cap wafer 310A and at least portions of the circuit/cap wafers 260A, where each of the cap wafer and the circuit/cap wafers that has recesses 320 (only one of which is shown in FIG. 14B) and standoff bumps 1215, is coated with an electrically conducting layer 350, and further has indium bumps 1284 connected to the electrically conducting layer through a Ti adhesion layer 1282. Note that the N circuit/cap wafers 260A are configured such that an area in the (x,y) plane, A(j), of the jth circuit/cap wafer 260A(j), where j=1 . . . N, increases from top to bottom: A(1)<A(2) < . . . <A(N). Moreover, area A(1) of the circuit/cap wafer 260A(1) adjacent to the cap wafer 310A is smaller than the area in the (x,y) plane of the cap wafer, and area A(N) of the circuit/cap wafer 260A(N) adjacent to the circuit wafer 210 equal to or larger than the area in the (x,y) plane of the circuit wafer.

The iteration of operations 1420 are performed bottom-to-top, in the following manner. As a first iteration of operation 1420, the circuit wafer 210 is cold bonded to the circuit/cap wafer 260A(N) by applying pressure P(N) to the circuit/cap wafer 260A(N) against the circuit wafer. Here, a value of the applied pressure is P(N)=F(N)/A(N), where F(N) is the force used to press on the circuit/cap wafer 260A(N) over its area A(N).

As a second iteration of operation 1420, the circuit/cap wafer 260A(N) is cold bonded to the circuit/cap wafer 260A(N−1) by applying pressure P(N−1) to the circuit/cap wafer 260A(N−1) against the circuit/cap wafer 260A(N). Here, a value of the applied pressure is P(N−1)=F(N−1)/A(N−1), where F(N−1) is the force used to press on the circuit/cap wafer 260A(N−1) over its area A(N−1). Because A(N−1)<A(N), a smaller force F(N−1)<F(N) is used to press on the circuit/cap wafer 260A(N−1) to obtain the same or slightly smaller bonding pressure P(N−1) P(N). And so on, in each additional step, the utilized bonding force is smaller than the previous one F(j−1)<F(j), where j=N . . . 1, and thus the bonding of the previous pair is not compromised. In some implementations, the relative magnitude of the force applied for consecutive iterations can be controlled by the relative height of the coated standoff bumps 1215, in the following manner. To insure that the condition F(j−1)<F(j) holds, the height H(j−1) of the coated standoff bumps 1215 for an iteration (j−1) has to be larger than the height H(j) of the coated standoff bumps 1215 for the previous iteration (j), where j=N . . . 1. In other words, the height of the coated standoff bumps 1215 decreases top-to-bottom, with the tallest coated standoff bumps 1215 between the cap wafer 310A and the circuit/cap wafer 260A(1), and the shortest coated standoff bumps 1215 between the circuit/cap wafer 260A(N) and the circuit wafer 210.

As the before last iteration of operation 1420, the circuit/cap wafer 260A(1) is cold bonded to the circuit/cap wafer 260A(2) by applying pressure P(1) to the circuit/cap wafer 260A(1) against the circuit/cap wafer 260A(2). Here, a value of the applied pressure is P(1)=F(1)/A(1), where F(1) is the force used to press on the circuit/cap wafer 260A(1) over its area A(1). Because A(1)<A(2), a smaller force F(1)<F(2) is used to press on the circuit/cap wafer 260A(1) to obtain the same or slightly smaller bonding pressure P(1) P(2).

As the last iteration of operation 1420, the cap wafer 310A is cold bonded to the circuit/cap wafer 260A(1) by applying pressure P(310A) to the cap wafer 310A against the circuit/cap wafer 260A(1). Here, a value of the applied pressure is P(310A)=F(310A)/A(310A), where F(310A) is the force used to press on the cap wafer 3100A over its area A(310A). Because A(310A)<A(1), a smaller force F(310A)<F(1) is used to press on the cap wafer 310A to obtain the same or slightly smaller bonding pressure P(310A) P(1).

Here, the number of N circuit/cap wafers 260A included in a 3D microwave integrated quantum circuit obtained using process 1410M can be N=1, as in the 3D microwave integrated quantum circuit 600AM, N=2, 3, 7, 15, 31 or other numbers.

FIG. 15 shows another example of a process 1500 for fabricating a 2D microwave integrated quantum circuit, e.g., like the 2D microwave integrated quantum circuit 600B described above in connection with FIG. 6B.

At 1510, a circuit wafer 210, a top cap wafer 310A and a bottom cap wafer 410A are received. Here, the circuit wafer 210 supports quantum circuit devices 240 (only one of which is shown in FIG. 15). Note that either of the processes 800 or 1300 can be used to fabricate via holes 330 in the circuit wafer 210. Moreover, a process similar to process 1200 has been used to fabricate the cap wafers 310A, 410A, each of which has recesses 320, 420 (only one of each is shown in FIG. 15), is coated with an electrically conducting layer 350, 450, and further has In balls 1286 connected to the electrically conducting layer.

As part of the receiving operation 1510, surfaces of the top cap wafer 310A and the bottom cap wafer 410A that are to be bonded can be cleaned using a plasma treatment.

These surfaces include surfaces of the In balls 1286 and areas of the electrically conducting layers 350, 450 adjacent to the In balls.

After the plasma treatment, the following alignments are performed: (i) the top cap wafer 310A is aligned relative to the circuit wafer 210, such that the In balls 1286 connected to the top cap wafer register to the top end of the via holes 330 of the circuit wafer; and (ii) the bottom cap wafer 410A is aligned relative to the circuit wafer 210, such that the In balls 1286 connected to the bottom cap wafer register to the bottom end of the via holes 330 of the circuit wafer.

At 1520, the circuit wafer 210, the top cap wafer 310A and the bottom cap wafer 410A are cold bonded together. Here, the bonding is performed using a press 1522, in which the top cap wafer 310A is pressed against the top surface of the circuit wafer 210, and the bottom cap wafer 410A is pressed against the bottom surface of the circuit wafer. Ductility of In (Mohs scale: 1.2) enables the In balls 1286 to deform (and not break) and fill the via holes 330 when the pressure is applied by the press 1522. In this manner, the top cap wafer 310, the circuit wafer 210 and the bottom cap wafer 410 are bonded together by the In that filled the via holes 330 to form In vias 1560. Note that the bonding operation 1520 is performed at temperatures that do not exceed 100° C., e.g., at temperatures less than 80° C.

The In vias 1560 also provide an electrical connection between the electrically conducting layers 350, 450 of the cap wafers 310, 410. In this manner, it is sufficient to provide a single ground connection to one of the electrically conducting layers 350, 450, and the other one of the electrically conducting layers 450, 350 will also be grounded through the In vias 1560.

FIG. 16 shows another example of a process 1600 for fabricating a 2D microwave integrated quantum circuit, e.g., like the 2D microwave integrated quantum circuit 600B described above in connection with FIG. 6B. Process 1600 includes the operations of process 1400 and an alignment step from process 1500.

At 1610, a circuit wafer 210, a top cap wafer 310A and a bottom cap wafer 410A are received. Here, the circuit wafer 210 supports quantum circuit devices 240 (only one of which is shown in FIG. 16). Note that process 1300 can be used to fabricate electrically conducting vias 560 in the circuit wafer 210. Moreover, a process similar to process 1200 has been used to fabricate the cap wafers 310A, 410A, each of which has recesses 320, 420 (only one of each is shown in FIG. 16), is coated with an electrically conducting layer 350, 450, and further has solder bumps 1288 connected to the electrically conducting layer. The solder bumps 1288 can include a solder alloy, e.g., an In-based solder alloy, such as In/Ga solder, that can be reflowed at low temperature. For example, In/Ga solder has meting temperature ˜16° C.

As part of the receiving operation 1610, surfaces of the top cap wafer 310A and the bottom cap wafer 410A that are to be bonded can be cleaned using a plasma treatment. These surfaces include surfaces of the solder bumps 1288 and areas of the electrically conducting layers 350, 450 adjacent to the solder bumps.

After the plasma treatment, the following alignments are performed: (i) the top cap wafer 310A is aligned relative to the circuit wafer 210, such that the solder bumps 1288 connected to the top cap wafer register to the top end of the electrically conducting vias 560 of the circuit wafer; and (ii) the bottom cap wafer 410A is aligned relative to the circuit wafer 210, such that the solder bumps 1288 connected to the bottom cap wafer register to the bottom end of the electrically conducting vias of the circuit wafer.

At 1620, the circuit wafer 210, the top cap wafer 310A and the bottom cap wafer 410A are bonded together by reflowing the solder bumps 1288. Here, the bonding is performed using a reflow apparatus 1622, to apply pressure and temperature for solder reflow. In this manner, the top cap wafer 310, the circuit wafer 210 and the bottom cap wafer 410 are bonded together by metal-metal bonds formed between caps of the electrically conducting vias 560 and the reflowed bumps 1288*. Note that the solder reflow operation 1520 is performed at temperatures that do not exceed 100° C., e.g., at temperatures less than 80° C.

The solder-capped vias (1288*-560-1288*) provide an electrical connection between the electrically conducting layers 350, 450 of the cap wafers 310, 410. In this manner, it is sufficient to provide a single ground connection to one of the electrically conducting layers 350, 450, and the other one of the electrically conducting layers 450, 350 will also be grounded through the solder-capped vias (1288*-560-1288*).

In some implementations, a 2D microwave integrated quantum circuit can be fabricated using cap wafers with mating features, such that In or solder bumps, electrically conductive vias are not required for assembling the 2D microwave integrated quantum circuit. An example of such a 2D microwave integrated quantum circuit is shown in FIG. 17A. FIG. 17 is a side view of an example of a 2D microwave integrated quantum circuit 1700 including a circuit wafer 210B, a top cap wafer 310B and a bottom cap wafer 410B that are arranged and configured like the corresponding components of the 2D microwave integrated quantum circuit 400 described above in connection with FIGS. 4A-4B.

However, the top cap wafer 310B has, in addition to structural and functional characteristics of the top cap wafer 310, a plurality of mating recesses 1744 (although only one is shown in FIG. 17A) that form a top cap pattern. Further, the bottom cap wafer 410B has, in addition to structural and functional characteristics of the bottom cap wafer 410, a plurality of mating protrusions 1742 that form a bottom cap pattern that is a “negative image” of the top cap pattern. Furthermore, the circuit wafer 210B has, in addition to structural and functional characteristics of the top circuit wafer 210, a plurality of openings 1746 (although only one is shown in FIG. 17A) arranged based on the bottom cap pattern. As such, the circuit wafer 210B is disposed over the bottom cap wafer 410 such that the mating protrusions 1742 protrude through the openings 1746. In this manner, the circuit wafer 210B and the bottom cap wafer 410B are secured together in the (x,y) plane. Moreover, the top cap wafer 310B is disposed over the circuit wafer 210B such that the mating recesses 1744 rest on top of the mating protrusions 1742 of the bottom cap wafer 410B. In this manner, the top cap wafer 310B and the circuit wafer 210B are secured together in the (x,y) plane.

Note that the mating protrusions 1742 and mating recesses 1744 form large contact surface areas which ensure, when compression along the z-axis is maintained on the 2D microwave integrated quantum circuit 1700, reliable DC (e.g., ground) and RF (e.g., signal) connections between at least portions of the electrically conducting layer 350 that coats the top cap wafer 310B and of the electrically conducting layer 450 that coats the bottom cap wafer 410B, without the use of solder bumps, In bumps, In vias, etc. In some implementations, cold welding may occur upon compressing the 2D microwave integrated quantum circuit 1700, for example, between when surfaces of the electrically conducting layers 350, 450 are covered with In.

FIG. 17B shows a process 1702 for fabricating the bottom cap wafers 410B using wet etching. In some implementations, wafers 1012 used for this process include an etch stopping layer 1018 for enhanced control of recess depth.

At 1710, a hard mask 912 (e.g., SiO_(x), SiN, etc.) is patterned on the wafer 1012 to define locations in the (x,y) plane of mating protrusions 1742 and their respective lateral sizes. Then, a soft mask 922 (e.g., a photoresist layer) is spin-coated on the patterned hard mask 912.

At 1720, the soft mask 922 is patterned to define locations in the (x,y) plane of the enclosure-forming recesses 420 and their width WW.

At 1730, the wafer 1012 is subjected to a first wet etch to form the enclosure-forming recesses 420. In other implementations, the first etch used to form the recesses enclosure-forming 420 can be DRIE. The depth of the first wet etch corresponds to the depth C_(h) of the recesses enclosure-forming 420. Then, the patterned soft mask 922 is removed.

At 1740, the wafer 1012 is subjected to a second wet etch to form the mating protrusions 1742. In other implementations, the second etch used to form the mating protrusions 1742 can be DRIE. The depth of the second wet etch, which may be controlled using the etch stopping layer 1018, corresponds to a height H_(P) of the mating protrusions 1742. The height HP of the mating protrusions 1742 is the sum of the depth C_(h) of the mating recesses 1744 and the thickness T of the circuit wafer 210, H_(P)=C_(h)+T. Then, the patterned hard mask 912 is removed.

At 1750, an electrically conducting layer 450 is coated on the wafer 1012 over the enclosure-forming recesses 420 and the mating protrusions 1742. Note that the bottom cap wafer 410B formed by using process 1702 has enclosure-forming recesses 420 of width WW and depth C_(h), has mating protrusions 1742 of height H_(P), and is coated with an electrically conducting layer 450. Moreover, the enclosure-forming recesses 420 are arranged in accordance with a pattern of the quantum circuit devices 240 supported on the circuit wafer 210B, and the mating protrusions 1742 are arranged in accordance with a predefined bottom cap pattern.

FIG. 17C shows a process 1705 for fabricating the top cap wafers 310A using wet etching. Process 1705 can be based on process 900 described above in connection with FIG. 9. Accordingly, Si wafers 916 can be used for process 1705.

At 1715, a single hard mask 912 (e.g., SiO_(x), SiN, etc.) is patterned on the Si wafer 916 to define locations in the (x,y) plane of the enclosure-forming recesses 320 and their width WW, and locations in the (x,y) plane of mating recesses 1744 and their respective lateral dimensions. Note that the locations in the (x,y) plane of mating recesses 1744 and their respective lateral dimensions matches the locations in the (x,y) plane of mating protrusions 1742 and their respective lateral dimensions defined at 1710 of process 1702.

At 1725, the Si wafer 916 is subjected to a wet etch to form the enclosure-forming recesses 320 and the mating recesses 1744. In other implementations, the etch used to form the enclosure-forming recesses 320 and the mating recesses 1744 can be DRIE. The depth of the wet etch corresponds to the depth C_(h) of the enclosure-forming recesses 320 and of the mating recesses 1744. Then, the patterned hard mask 912 is removed.

At 1735, an electrically conducting layer 350 is coated on the Si wafer 916 over the enclosure-forming recesses 320 and the mating recesses 1744. Note that the top cap wafer 310B formed by using process 1705 has enclosure-forming recesses 320 of width WW and depth C_(h), has mating protrusions 1742 of depth C_(h), and is coated with an electrically conducting layer 350. Moreover, the enclosure-forming recesses 320 are arranged in accordance with the pattern of the quantum circuit devices 240 supported on the circuit wafer 210B, and the mating recesses 1744 are arranged in accordance with a predefined top cap pattern that matches the bottom cap pattern.

FIG. 18 is a side view of another example of a 2D microwave integrated quantum circuit 1800 including a circuit wafer 210C, a top cap wafer 310C and a bottom cap wafer 410C that are arranged and similar to the corresponding components of the 2D microwave integrated quantum circuit 400 described above in connection with FIGS. 4A-4B.

However, although the height Cht of recesses 1844 of the top cap wafer 310C is the same as the height of the recesses of the top cap wafer 310, a width of the recesses 1844 is (WW+2WP). Further, bottom cap wafer 410C has a plurality of pairs of mating protrusions 1842, each pair corresponding to a quantum circuit device 240 and defining a recess 1845. Each mating protrusion 1842 has a width WP. Additionally, the recess 1845 has a depth equal to the sum (Cht+T+Chb), where T is the thickness of the circuit wafer 210C and Chb equals the height of the recesses of the bottom cap wafer 410. Here, the recesses 1844 of the top cap wafer 310C and the recesses 1845 of the bottom cap wafer 410C correspond to the quantum circuit device 240 supported on the circuit wafer 210C. Furthermore, the circuit wafer 210C has, in addition to structural and functional characteristics of the circuit wafer 210, a plurality of openings of width WP through which the mating protrusions 1842 penetrate as the circuit wafer rests on the bottom cap wafer 410C. In this manner, the circuit wafer 210C and the bottom cap wafer 410C are secured together in the (x,y) plane. Moreover, the top cap wafer 310C is disposed over the circuit wafer 210C such that the recesses 1844 rest on top of the mating protrusions 1842 of the bottom cap wafer 410C. In this manner, the top cap wafer 310C and the circuit wafer 210C are secured together in the (x,y) plane.

Note that the mating protrusions 1842 and mating recesses 1844 form large contact surface areas to ensure, when compression along the z-axis is maintained on the 2D microwave integrated quantum circuit 1800, reliable DC (e.g., ground) and RF (e.g., signal) connections between at least portions of the electrically conducting layer 350 that coats the top cap wafer 310C and of the electrically conducting layer 450 that coats the bottom cap wafer 410C, without the use of solder bumps, In bumps, In vias, etc. In some implementations, cold welding may occur upon compressing the 2D microwave integrated quantum circuit 1800, for example, between when surfaces of the electrically conducting layers 350, 450 are covered with In.

A main distinction between the cap wafers 310B, 410B of the 2D microwave integrated quantum circuit 1700 the cap wafers 310C, 410C of the 2D microwave integrated quantum circuit 1800 is that the former have mating recesses 1744 and protrusions 1742 that are spaced apart from the enclosure-forming recesses 320, 420, while the latter have mating recesses 1844 and protrusions 1842 that help define the enclosure-forming recesses 320, 420.

The cap wafers 310C, 410C can be fabricated using any of the processes 900, 1000, 1100 and 1150 described above in connection with FIGS. 9, 10, 11A and 11B, respectively.

As discussed previously, in general, quantum computing systems 100 can include a signal delivery system 106 to deliver signals between a control system 110 and a quantum processor cell 102. In many implementations, the signal delivery system 106 includes an interposer for electrically routing signal pads on an exterior surface of a circuit wafer 210 to cable connectors. For example, referring to FIG. 19, a quantum computing apparatus 1900 includes a quantum circuit device 1910 attached to an interposer 1920. Interposer 1920 connects quantum circuit device 1910 to a series of cables 1950, which connect the quantum computing apparatus 1900 to a control system (not shown).

Generally, an interposer is a multi-layer device that includes electrical contacts on one surface that are connected to signal lines that fan out, through the layers, to the electrical connectors, e.g., on the opposing side of the interposer. The electrical contacts on the interposer have the same layout as the contact electrodes on the circuit wafer to that, when attached to the circuit wafer, the interposer provides electrical conduction paths from the cable connectors to the quantum circuit device. By fanning the signal lines out, the interposer facilitates connection of conventional cabling (e.g., RF coaxial cables) to the micro circuitry of the quantum computing device. Generally, the interposer includes at least one electrically insulating substrate layer with through holes (e.g., laser drilled or etched, such as DRIE etched) for the signal lines. Common materials for the substrate layer include silicon, BeO, Al₂O₃, AlN, quartz, sapphire, and PCB. The signal lines can be formed by coating the via holes with a conductive film (e.g., a normal conductor or superconductor).

Typically, the interposer also includes a conductive film (e.g., a normal conductor or superconductor), often metal (e.g., indium, aluminum, tin), deposited on a surface of the substrate layer. These films can be formed on the substrate layer in a variety of ways, such as by sputtering, evaporation, or electroplating. Typically, the conductive layer is patterned using a conventional patterning technique (e.g., wet etching, dry etching, lift off, laser writing, milling, screen printing, etc.).

In many cases, the interposer includes more than one substrate layers bonded together. For example, the interposer 1920 depicted in FIG. 19 includes intermediate layers 1930 (e.g., one or more layers) and a connectorization layer 1940. Intermediate layers 1930 includes signal lines connecting electrical contacts on the surface of quantum circuit device 1910 facing interposer 1920 with connectorization layer 1940 in addition to circuitry (e.g., integrated circuitry) for performing one or more of a variety of functions, such as amplifying signals, multiplexing or de-multiplexing signals, routing signals, etc.

Connectorization layer 1940 provides mechanical support for the intermediate layers of interposer 1920 and includes connectors for cables 1950, along with signal lines connecting the cable connectors to the signal lines of intermediate layers 1930.

Before turning to exemplary embodiments of interposers, it is noted that a variety of circuit wafer structures may be used to reliably attach the circuit wafer to the interposer. For example, in some embodiments a pattern layer of aluminum can be provided on the lower surface of a circuit wafer for attachment to an interposer. Specifically, referring to FIG. 20A, a quantum computing apparatus 2000 includes a quantum circuit device 2010 and an interposer 2020. The quantum circuit device 2010 includes a circuit wafer 2014, which supports a quantum circuit 2012 on one surface, and a patterned aluminum layer—depicted as portions 2016 and 2018—on the opposing surface. The patterned aluminum layer provides electrical contacts to signal lines (e.g., through vias) in circuit wafer 2014. The patterned aluminum layer can be formed by natively growing a layer of aluminum on the surface of circuit wafer 2014 and then patterning the layer using conventional lithographic techniques. The interposer 2020 may then be bonded to the patterned aluminum layer using conventional bonding techniques, such as wire bonding, ball bonding, etc.

Of course, while FIG. 20A depicts only a single quantum circuit and a pair of aluminum portions, in general the circuit wafer can support numerous quantum circuits and aluminum portions. Moreover, while quantum circuit device 2010 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Other circuit wafer structures for interposer attachment may also be used. For example, referring to FIG. 20B, a quantum computing apparatus 2000′ includes a quantum circuit device 2010′ and interposer 2020. Quantum circuit device 2010′ includes quantum circuit 2012, circuit wafer 2014, and portions 2016 and 2018 of a patterned aluminum layer. This surface also includes a passivation layer 2030 and a patterned layer of a solderable metal (e.g., Pt, Au, or Pd) including portions 2032 and 2034. Portion 2032 is registered and in contact with Al portion 2016, providing an electrical contact to signal lines in circuit wafer 2014. Similarly, Portion 2034 is registered and in contact with Al portion 2018, providing another electrical contact.

In general, at least one of the layers of the interposer provides a substrate for supporting other layers and/or connectors. The interposer substrate material can be silicon, sapphire, ceramic, printed circuit board (PCB) or other material that is sufficiently mechanically robust and compatible with the other layers, manufacturing techniques, and operational conditions of the quantum computing apparatus.

In general, interposers suitable for a quantum circuit device should include some (e.g., all) of the following attributes. First, the interposer should be compatible with the operational temperature of the quantum computing device, i.e., cryogenic temperatures, such as liquid helium temperature. The interposer should also be sufficiently robust to endure the same thermal cycling as the quantum computing device (e.g., cycling between room temperature and cryogenic temperatures). Thermal robustness may be achieved by forming the interposer from a material that has a similar (e.g., the same) coefficient of thermal expansion as the circuit wafer (e.g., silicon) so that any expansion or contraction of the circuit wafer is matched by the interposer during thermal cycling.

The interposer materials should also have relatively low microwave loss, specifically at the operational frequencies of the quantum circuit device.

The layers forming the interposer should have relatively flat surfaces in order to facilitate accurate registration of features (e.g., electrical contacts) between different layers and/or to the quantum circuit device. Specifically, surfaces should have sufficiently smooth, planar surfaces so that reliable and robust connections can be made between contact electrodes on opposing surfaces. In some embodiments, surfaces can have a Ra value of 5 μm or less (e.g., 2 μm or less, 1 μm or less, 500 nm or less, 200 nm or less).

Furthermore, the materials forming the interposer should be compatible with the processes used to form and package the quantum circuit device. For instance, materials should be compatible with conventional integrated circuit forming and packaging techniques, including photolithography, deposition of metal and passivation layers, polishing (e.g., chemical mechanical polishing), and etching (e.g., reactive ion etching) techniques.

Example materials for use in the interposer include silicon, sapphire, ceramics (e.g., alumina, aluminum nitride), printed circuit boards (PCB), Kapton, polyimide, and deposited layers such as SiO₂ and Si₃N₄.

Moreover, in addition to forming the interposer from materials that are compatible with the quantum circuit device, compatible layer bonding techniques should also be used. In general, bonding should provide sufficiently robust attachment between layers to maintain good contact between contact electrodes on adjacent surfaces. Typically, bonding will depend on the materials (e.g., metals) being bonded. In many cases, wafer bonding techniques are applied. For example, in some embodiments, bonding can be achieved using indium bumps or indium balls. The indium can be patterned using lift off or screen printing techniques. Indium bonding can be achieved using force-only, low temperature or high temperature bonding.

In certain embodiments, bonding is achieved using solder bumps or solder balls, e.g., patterned using a screen printing process. Such bonding can also be achieved used high temperature or low temperature bonding. Aluminum bonding at high or low temperature can also be used. Alternatively, or additionally, connection of contact electrodes between adjacent surfaces can be enabled by mechanical connections, such as using pins (e.g., pogo pins), fuzz buttons, and/or with tips covered with diamond nanoparticles.

Wire-bonding can also be used. For example, the interposer substrate layer(s) can include one or more physical holes acting as pass-thrus for wire bonds from the interposer to the back surface of the quantum circuit device. In some embodiments, the chip stack of the quantum circuit device is assembled onto a carrier, e.g., a substrate formed from aluminum, molybdenum, copper, etc. The chip stack can be glued onto the carrier using an adhesive material, such as an epoxy, eccosorb, etc. The carrier can provide pressure relief by use of compressible or spring-like material, such as fuzz buttons, copper wool, brass wool, gold wool, etc. The carrier can be mounted on a PCB using, e.g., alignment pins and registration marks. In some embodiments, a back plate forms an electromagnetic closure on the opposite side of the PCB from the chip stack and carrier. For example, lossy microwave material can be integrated into the assembly formed by the chip stack, carrier, and PCB. In some implementations, oxygen-free high thermal conductivity (OFHC) copper can be used.

In general, the signal lines provide electrical connections for DC signals, RF signals, and/or ground connections. In various embodiments, the interposer is composed of PCB that includes multiple layers of metal (e.g., 3-30 metal layers). The PCB can include thru and blind vias between the metal layers. RF signals may be routed on a particular metal layer of the PCB, and wire bonds for RF signals make connections from that metal layer to the back plane of the chip stack. DC or low frequency signals may be routed on a different metal layer from the RF signals. Wire bonds from the DC/LF metal layer may also form connections from that layer to the back plane of the chip stack.

Turning now to specific examples of interposers and referring to FIG. 21, a quantum computing apparatus 2100 includes a quantum circuit device 2110 and a multilayer interposer 2180 for connecting the quantum circuit device to cables 2170. Quantum circuit device 2110 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2118 and an N-th circuit wafer 2120. Each circuit wafer supports a quantum circuit, including quantum circuit 2116 which is supported by circuit wafer 2118 and quantum circuit 2122 supported by circuit wafer 2120. A cap wafer 2112 encloses quantum circuit 2116 in a cavity 2114 (which may also be referred to as a pocket or enclosure). While quantum circuit device 2110 is depicted with minimal structure, it will be understood that any of the microwave quantum integrated circuits described above can be used.

Interposer 2180 is a multi-layer scalable interposer that includes a routing layer 2130, a directional coupling layer 2140, a layer 2150 that includes quantum amplifiers and multiplexers, and a connectorization layer 2160 having connectors for cables 2170. Routing layer 2130, directional coupling layer 2140, and a layer 2150 each include integrated circuits for performing the functions associated with that layer. Additional layers with integrated circuitry may be included between layer 2150 and connectorization layer 2160. Each layer may include its own substrate or may be mechanically supported on a substrate of another layer. Suitable substrate materials include silicon, ceramic, sapphire, and PCB.

The layers of interposer 2180 are bonded together using bonding materials and techniques suitable for the two layers being attached. For example, ball bonding, solder bonding, or spring loaded connections may be used.

In some embodiments, the interposer can include one or more ceramic layers (e.g., alumina or AlN). For example, referring to FIG. 22, a quantum computing apparatus 2200 includes a quantum circuit device 2210 and an interposer 2280 including a ceramic layer 2240 for connecting the quantum circuit device to cables 2270.

Quantum circuit device 2210 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2218 and an N-th circuit wafer 2220. Each circuit wafer supports a quantum circuit, including quantum circuit 2216 which is supported by circuit wafer 2218 and quantum circuit 2222 supported by circuit wafer 2220. A cap wafer 2212 encloses quantum circuit 2216 in a cavity 2214. While quantum circuit device 2210 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Certain ceramics have coefficients of thermal expansion (CTE's) which are close to the CTE of silicon over temperature ranges spanning from cryogenic temperatures (e.g., liquid Helium temperatures) to room temperature, and are therefore promising candidates for bonding to silicon circuit wafers. For instance, alumina has a CTE of 6-7 ppm/° C. and AlN has a CTE of 4 ppm/° C. while silicon has a CTE of 2.6 ppm/° C. Ceramics such as alumina and AlN have relatively low microwave attenuation. Moreover, ceramic layers can be formed with relatively flat surfaces, e.g., having a Ra of about 1 μm or less.

Ceramic layer 2240 may be in the form of a thick film having a thickness in a range of about 25-30 mils, for instance.

A variety of methods can be used to form ceramic layer 2240. For example, in some implementations, ceramic layer 2240 is formed using a low temperature co-firing process to form a low temperature co-fired ceramic (LTCC) layer. Typically, LTCC technology involves the production of multilayer circuits from ceramic substrate tapes or sheets. Conductive, dielectric, and/or resistive pastes can be applied on each sheet or tape, and then the sheets/tapes are laminated together and fired in one step. The resulting layer is a hermetic, monolithic structure. A typical LTCC structure has multiple dielectric layers, screen-printed or photo-imaged low-loss conductors, and viaholes for interconnecting the multiple layers. Alternatively, thick film processes that involve applying conductive or dielectric pastes on top of a thick ceramic substrate and firing them together can be used. Similar to LTCC, conductors may be screen-printed or photo-imaged to achieve desired feature sizes.

Ceramic layer 2240 is ball-bonded to circuit wafer 2220 using solder balls of, e.g., low temperature indium or other low temperature solder alloys. For example, the layers can be bonded together by placing the balls on the top surface of ceramic layer 2240 and bonding the surface of circuit wafer 2220 to the balls using a low temperature indium or solder bonding process, forming a permanent bond between the circuit wafer and the ceramic layer.

In addition to ceramic layer 2240, interposer 2280 includes a thinnerposer 2250 and connectorization layer 2260, providing connection to cables 2270. Thinnerposer 2250 includes electrically conducting fuzzbutton interconnects 2252 embedded in a dielectric substrate. Thinnerposers offer low signal distortion, robustness, and consistency and are commercially available from Custom Interconnects (Centennial, Colo.).

In some implementations, interposers can use wire bonding to connect to a circuit wafer. For example, referring to FIG. 23, a quantum computing apparatus 2300 includes a quantum circuit device 2310 and an interposer 2380 for connecting, using wire bonds, the quantum circuit device to cables 2370. Quantum circuit device 2310 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2318 and an N-th circuit wafer 2320. Each circuit wafer supports a quantum circuit, including quantum circuit 2316 which is supported by circuit wafer 2318 and quantum circuit 2322 supported by circuit wafer 2320. A cap wafer 2312 encloses quantum circuit 2316 in a cavity 2314. While quantum circuit device 2310 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Interposer 2380 is a multi-layer interposer formed from four PCB layers 2340, a thinnerposer 2350, and a connectorization layer 2360 for connecting the quantum circuit device to cables 2370.

Each PCB layer includes metalized surfaces (e.g., 2341) for bonding and forming signal lines. Vertical metallic interconnects (e.g., via 2342) run through the PCB layers in the z-direction, connecting the signal lines through to the lower surface of PCB layers 2340. Wires 2332 bonded at one end to a conducting metal layer on a PCB layer and to an electrode 2330 on circuit wafer 2320 connect the signal lines to the quantum computing device 2310. Each PCB layer includes an aperture registered with apertures on the other layers and thus providing a through hole for threading the wires and providing access to circuit wafer 2320.

Thinnerposer 2350 includes fuzz buttons registered with electrical contacts on the underside of the PCB layers 2340 on one side, and registered with electrical contacts connected to cables 2370 on the other side.

In some implementations, the interposer can include multiple substrate layers of silicon. For example, referring to FIG. 24, a quantum computing apparatus 2400 includes a quantum circuit device 2410 and an all-silicon interposer 2480 for connecting, using wire bonds, the quantum circuit device to cables 2470. Quantum circuit device 2410 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2418 and an N-th circuit wafer 2420. Each circuit wafer supports a quantum circuit, including quantum circuit 2416 which is supported by circuit wafer 2418 and quantum circuit 2422 supported by circuit wafer 2420. A cap wafer 2412 encloses quantum circuit 2416 in a cavity 2414. While quantum circuit device 2410 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Interposer 2480 includes three stacked silicon layers 2440, 2445, and 2450 and a silicon connectorization layer 2460. Layer 2440 includes routing circuitry, layer 2445 includes directional coupling circuitry, and layer 2450 includes quantum amplification circuitry and multiplexing circuitry. Additional silicon layers can also be included, e.g., between layer 2450 and connectorization layer 2460. The silicon substrates can be fabricated with standard silicon microfabrication techniques, such as silicon DRIE for vias, metal sputtering, photolithography, etc. Generally, metallization can be any non-magnetic metal, preferably superconducting at the operational temperature of quantum computing apparatus 2400.

The silicon layers are bonded together using low temperature wafer bonding using indium bumps or indium balls, discussed above. In order to bond more than two silicon layers using low temperature indium bonding, the bonding may be performed bottom to top, the bottom being connectorization layer 2460, and the top being cap wafer 2412 of quantum circuit device 2510. In order to fan out the signal lines, the area of the layers of interposer 2480 increase as they proceed to connectorization layer 2460. By bonding the largest layers first (i.e., those at the bottom of the structure), the bonding utilizing the largest bonding force occurs earlier in the process. Sequentially bonding subsequent smaller layers uses less bonding force, meaning there is less chance that the structure will be comprised during formation as the number of layers increase. This can improve yields. Other advantages of indium bonding multiple silicon layers for form an interposer include CTE match to the quantum circuit device, low microwave loss of the structure, and planarity of the surfaces.

Alternatively, or additionally, indium bonding can also be used to bond silicon layers in the interposer. For example, referring to FIG. 25, a quantum computing apparatus 2500 includes a quantum circuit device 2510 and an interposer 2580 having silicon layers bonded using indium for connecting the quantum circuit device to cables 2570. Quantum circuit device 2510 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2518 and an N-th circuit wafer 2520. Each circuit wafer supports a quantum circuit, including quantum circuit 2516 which is supported by circuit wafer 2518 and quantum circuit 2522 supported by circuit wafer 2520. A cap wafer 2512 encloses quantum circuit 2516 in a cavity 2514. While quantum circuit device 2510 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Interposer 2580 includes three stacked silicon layers 2540, 2550, and 2560. Additional silicon layers can also be included, e.g., between layers 2550 and 2560. Vias 2545 are also shown for each of silicon layers 2540, 2550, and 2560. These layers are bonded using aluminum bonding. This involves metallization of each surface of silicon layers 2540, 2550, and 2560 with aluminum, patterning the aluminum layer to provide contacts 2532, and bonding the contacts of adjacent layers with bonding balls 2530.

Interposer 2580 also includes a thinnerposer 2565 and a connectorization layer 2570, connected to cables 2575. Thinnerposer 2565 includes fuzz buttons registered with corresponding aluminum contacts on silicon layer 2560 and with cable connectors on connectorization layer 2570.

Aluminum metallization can also be used for bonding silicon layers together. For example, referring to FIG. 26, a quantum computing apparatus 2600 includes a quantum circuit device 2610 and an interposer 2680 for connecting the quantum circuit device to cables 2670. Quantum circuit device 2610 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2618 and an N-th circuit wafer 2620. Each circuit wafer supports a quantum circuit, including quantum circuit 2616 which is supported by circuit wafer 2618 and quantum circuit 2622 supported by circuit wafer 2620. A cap wafer 2612 encloses quantum circuit 2616 in a cavity 2614. While quantum circuit device 2610 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Interposer 2680 includes three stacked silicon layers 2640, 2640, and 2650 and a silicon connectorization layer 2460. Additional silicon layers can also be included, e.g., between layer 2450 and connectorization layer 2460. Layer 2640 includes routing circuitry, layer 2640 includes directional coupling circuitry, and layer 2650 includes quantum amplification circuitry and multiplexing circuitry. Additional silicon layers may be included, e.g., between layer 2650 and connectorization layer 2660, which connects to cables 2670.

Each of the silicon layers includes aluminum metallization on its opposing surfaces, patterned to form electrodes. Aluminum electrodes 2632 on the top surface of layer 2630 are registered and bonded with aluminum electrodes 2624 on the bottom surface of circuit wafer 2620. Aluminum electrodes 2642 on the top surface of layer 2640 are registered and bonded with aluminum electrodes 2634 on the bottom surface of layer 2630. Similarly, aluminum electrodes 2652 on the top surface of layer 2650 are registered and bonded with aluminum electrodes 2644 on the bottom surface of layer 2430. Electrodes 2662 on the top surface of connectorization layer 2660 are also shown. These are registered and bonded with corresponding electrodes on the bottom surface of the adjacent silicon layer. In each case, low temperature covalent bonding with ion milling can be used to ensure robust bonding between the aluminum electrodes.

In some embodiments, integrated circuit layers of the interposer can be integrated directly onto a circuit wafer of the quantum computing device. For example, referring to FIG. 27, a quantum computing apparatus 2700 includes a quantum circuit device 2710 and an interposer 2780 for connecting the quantum circuit device to cables 2770. Quantum circuit device 2710 is a 3D device composed of multiple, stacked circuit wafers including a first circuit wafer 2718 and an N-th circuit wafer 2720. Each circuit wafer supports a quantum circuit, including quantum circuit 2716 which is supported by circuit wafer 2718 and quantum circuit 2722 supported by circuit wafer 2720. A cap wafer 2712 encloses quantum circuit 2716 in a cavity 2714. While quantum circuit device 2710 is depicted with minimal structure, it will be understood that any of the microwave integrated quantum circuits described above can be used.

Interposer 2780 includes a routing circuit layer 2730 formed on the surface of the lowest (Nth) circuit wafer 2720. A direction coupling layer 2740 is formed on the routing circuit layer 2730, and a multiplexing circuit layer 2750 is formed on the direction coupling layer 2740. Passivation layers may be provided between circuit wafer 2720 and routing circuit layer 2730, between routing circuit layer 2730 and direction coupling layer 2740, and/or between direction coupling layer 2740 and multiplexing circuit layer 2750. Suitable materials for passivation layers include silicon oxide, which may be deposited, or organic materials like polyimides, which may be spin coated. Such structures may be formed by sequentially depositing, patterning, and planarizing each layer using conventional semiconductor manufacturing methods. In the above description, numerous specific details have been set forth in order to provide a thorough understanding of the disclosed technologies. In other instances, well known structures, interfaces, and processes have not been shown in detail in order to avoid unnecessarily obscuring the disclosed technologies. However, it will be apparent to one of ordinary skill in the art that those specific details disclosed herein need not be used to practice the disclosed technologies and do not represent a limitation on the scope of the disclosed technologies, except as recited in the claims. It is intended that no part of this specification be construed to effect a disavowal of any part of the full scope of the disclosed technologies. Although certain embodiments of the present disclosure have been described, these embodiments likewise are not intended to limit the full scope of the disclosed technologies.

FIG. 28 is a schematic diagram of example multi-layer material stacks 2811, 2821 on an example cap wafer 2810 and circuit wafer 2820. In some cases, the stacks 2811, 2821 shown in FIG. 28 may be formed using one or more of the processes described above. In the example shown, the cap wafer 2810 has a multi-layer material stack 2811 disposed on its lower side and the circuit wafer 2820 has a multi-layer material stack 2821 disposed on its upper side, such that the stacks 2811, 2821 face each other. In some implementations, the stacks 2811, 2821 include a combination of superconducting material layers and non-superconducting material layers, yet maintain one or more superconducting properties. In some implementations, the stacks 2811, 2821 are bonded together to form a bonded multi-layer material stack that maintains superconducting properties despite including non-superconducting material layers (e.g., through the proximity effect). Once bonded together, current may flow perpendicular to the layers of the bonded stack (in the direction shown in FIG. 6) to provide a lossless connection between circuit elements on the cap wafer and circuit elements on the circuit wafer. The stacks 2811, 2821 may be implemented as an electrically conducting layer between wafers in a microwave integrated quantum circuit. For example, one or more of the electrically conducting layers described above (e.g., electrically conducting layers 350, 450) may be implemented similarly to either or both of stacks 2811, 2821.

In the example shown, the stack 2811 includes a layer 2812 of aluminum, a layer 2814 of molybdenum, a layer 2816 of titanium, and a layer 2818 of indium, and the stack 2821 includes a layer 2822 of aluminum, a layer 2824 of titanium, and a layer 2826 of palladium. In some implementations, the combined thickness of the layers 2812, 2814 is between approximately 0.5-2 μm, and the thickness of the respective layers can be divided in various ways between the two materials. In some instances, such as when the layer 2814 includes molybdenum, the layer 2814 may be approximately 200 nm thick. Where the layer 2814 includes molybdenum, the layer may produce a conductive oxide, which may facilitate superconductivity through proximity effect with non-superconducting layers in the stack. However, in instances where the layer 2814 includes a non-superconducting material, the layer 2814 may be less than 60 nm thick (to allow for the stack to still exhibit superconducting properties through the proximity effect, as described below). In some implementations, the thickness of layer 2816 is between 0 nm and 35 nm, such as, for example, 30 nm. In some implementations, the thickness of layer 2818 is between 3 μm and 10 μm, such as, for example approximately 6 μm. In some implementations, the layer 2822 may have a thickness between approximately 50-300 nm, the layer 2824 may have a thickness between approximately 2-5 nm, and the layer 2826 may have a thickness between approximately 30-60 nm. In some implementations, the layer 2826 may have a thickness between approximately 40-70 nm (thicknesses greater than 40 nm may allow for visibility as an alignment mark, while thicknesses greater than 70 nm may limit the proximity effect).

Although FIG. 28 depicts the multilayer stack 2811 of the example cap wafer 2810 has as having four layers and the multilayer stack 2821 of the circuit wafer as having three layers. This depiction is not intended as limiting. The multilayer stacks 2811, 2821 may have any number of layers provided the number maintains the one or more superconducting properties.

For example, the multilayer stack 2811 of the cap layer 2810 may have four layers formed of, respectively, niobium, an alloy of titanium and tungsten (e.g., TiW), niobium, and an alloy of molybdenum and rhenium. The first layer of niobium may be in contact with the cap wafer 2810 and the layer of molybdenum and rhenium may be an outer layer of the multilayer stack 2811. The layer of titanium and tungsten may be sandwiched between the first and second layers of niobium. The first layer of niobium may act as an adhesion layer for adhesion of the layer of titanium and tungsten to the cap wafer 2810. However, the first layer of niobium may suffer from copper inter-diffusion, such as from an underlying through-silicon via (TSV). As such, the first layer of niobium may lose its capability to become superconducting (or become degraded in its ability to superconduct). The layer of titanium and tungsten is present as a diffusion barrier to prevent copper from diffusing further into the second layer of niobium. The second layer of niobium may thus serve as a primary carrier of superconducting electrical current, through which, signals propagate through the cap wafer 2810. The layer of molybdenum and rhenium is present as a diffusion barrier to oxygen, preventing the oxidization of the underlying second layer of niobium.

It will be appreciated that the first layer of niobium improves the adhesion of the layer of titanium and tungsten and prevents delamination of that layer. The layer of titanium and tungsten prevents copper diffusion into the superconducting signal carrier layer, i.e., the second layer of niobium, which is critical to signal integrity. The layer of titanium and tungsten is not superconducting, but its thickness is tuned such that superconducting signals can be exchanged between the first and second layers of niobium through the Holm-Meissner proximity effect (and subsequently from the first layer of niobium to copper-containing through-silicon vias). The layer of molybdenum and rhenium, which serves as a passivation layer, adds to the robustness of the multilayer stack 2811 by preventing the formation of metal oxides and allowing the first and second layers of niobium to survive through high heat processes.

It will be understood that the quantum circuits on the circuit wafer 2820 are electromagnetically shielded from elements formed from non-superconducting copper (e.g., TSVs). Normal metals such as copper can disrupt a quantum coherence of a superconducting metal used to form and connect the quantum circuits. The second layer of niobium is used for this shielding. As mentioned above, the second layer of niobium is kept substantially copper-free by the layer of titanium and tungsten, which serves as a diffusion barrier. All metal layers (other than copper) are deposited in-situ without breaking vacuum. All metal layers are also patterned in the same lithography step, and subsequently etched in a single dry etch step. This greatly reduces processing times and complexity, and prevents the formation of interfacial metal oxides.

In this example, the multilayer stack 2821 of the circuit wafer 2820 may be two layers formed of, respectively, (1) an alloy of molybdenum and rhenium and (2) niobium. The layer of niobium may be in contact with the circuit wafer 2820 and the layer of molybdenum and rhenium may be an outer layer of the multilayer stack 2821. In some instances, the alloy of molybdenum and rhenium may have the same composition between in the multilayer stacks 2811, 2821. In other instances, the alloy of molybdenum and rhenium have a different composition in the multilayer stacks 2811, 2821.

In another example, the multilayer stacks 2811, 2821 may each have two layers, one formed of niobium and another formed of an alloy of molybdenum and rhenium. The layers of niobium may be, respectively, in contact with the cap wafer 2810 and the circuit wafer 2820 while the layers of molybdenum and rhenium may be outer layers of the multilayer stacks 2811, 2821. In some instances, the alloy of molybdenum and rhenium may have the same composition in the multilayer stacks 2811, 2821. In other instances, the alloy of molybdenum and rhenium have a different composition in the multilayer stacks 2811, 2821.

In the example shown, the cap wafer 2810 and circuit wafer 2820 are bonded together to form a microwave integrated quantum circuit. In some instances, to bond the wafers 2810, 2820 together, the cap wafer 2810 and the circuit wafer 2820 may be bonded together by applying a force to the cap wafer 2810 as shown in FIG. 28 until the multi-layer material stack 2811 meets and bonds with the multi-layer material stack 2821 on the circuit wafer 2820. In some implementations, the force applied may be approximately equivalent to 45 kg. In some instances, the surface area of the layer 2818 is between approximately 2-11 mm² and the force applied to the cap wafer 2810 exerts a pressure on the material layer stacks that is between 40-220 MPa. In some implementations, the bonding process takes place at a temperature between approximately 65-70° C., since, in some cases, higher temperatures may cause damages to Josephson junctions formed on the cap wafer 2810 or circuit wafer 2820. In some instances, the bonding process may occur at or near room temperature to reduce or avoid oxidation on the layers of the stacks 2811, 2821. In such instances, the force applied to the cap wafer 2810 may be greater than 45 kg to ensure proper bonding between the stacks 2811, 2821 (since lower temperatures may require higher amounts of force to be applied to the cap wafer to deform the materials of stacks 2811, 2821 and bond the wafers).

When bonded together, the stacks 2811, 2821 may form a multi-layer material stack that provides a zero resistance or near-zero resistance conductive path at low temperatures (e.g., cryogenic temperatures). In some cases, although the layer 2826 is composed of a non-superconducting material (e.g., palladium in the example shown), the bonded stacks 2811, 2821 may still exhibit superconducting properties. For example, the bonded stacks 2811, 2821 may have a resistance that is zero or approximately zero, such as less than 1 mΩ, when subjected to temperatures below the constituent materials' critical temperatures (e.g., at or below 100, 10, or 1 K), depending on the critical temperature of the materials in the bonded stacks). Thus, although the bonded stacks include one or more non-superconducting materials, the bonded stacks may act similarly to a stack that contains only superconducting materials. The bonded stack may exhibit such superconducting properties because of the proximity effect, which is the phenomenon where the superconductivity of a superconducting material “extends” into a non-superconducting material (e.g., based on Andreev reflection). With the proximity effect, the superconducting order may decay exponentially as a function of the distance into the non-superconducting material, with a decay constant on the order of tens of nanometers (which may depend on the conductivity of the non-superconducting material). A material such as palladium (or another material that is, like palladium, non-oxidizing and dense enough to be visible as an alignment mark in an electron-beam lithography tool; e.g., gold or platinum) may be chosen for use in the layer 2826 because it can be deposited using evaporation techniques and is conductive enough to obtain superconductivity through the proximity effect discussed above. In addition, palladium, gold, platinum, or another similar material may be chosen for layer 2826 because of its oxidation-resistive properties.

Although shown in FIG. 28 as including particular materials, the multi-layer material stacks 2811, 2821 may include other materials or compounds. For example, a number of different superconducting materials may be used in place of the aluminum of layers 2812, 2822, such as, for example, niobium, titanium nitride, molybdenum, or vanadium. As another example, palladium, gold, platinum, or alloys such as an alloy of molybdenum and rhenium (which may be more resistant to oxidation than molybdenum) can be used in place of the molybdenum in layer 2814. In addition, another type of non-oxidizing material that can be deposited via conformal deposition methods (e.g., sputtering, atomic layer deposition, or chemical vapor deposition), and can be thin enough to maintain a proximity effect, may be used in place of the molybdenum in layer 2814. As yet another example, platinum or gold may be used in place of the palladium in layer 2826. As yet another example, gallium may be used in place of the indium in layer 2818. In such instances, because gallium's melting point is approximately 30 degrees Celsius, the bonding process may occur below 30 degrees Celsius (e.g., at or near room temperature). Furthermore, although a number of layers are shown in the stacks 2811, 2821, fewer or additional material layers than those illustrated may be used.

While this specification contains many details, these should not be understood as limitations on the scope of what may be claimed, but rather as descriptions of features specific to particular examples. Certain features that are described in this specification or shown in the drawings in the context of separate implementations can also be combined. Conversely, various features that are described or shown in the context of a single implementation can also be implemented in multiple embodiments separately or in any suitable subcombination.

Similarly, while operations are depicted in the drawings in a particular order, this should not be understood as requiring that such operations be performed in the particular order shown or in sequential order, or that all illustrated operations be performed, to achieve desirable results. In certain circumstances, multitasking and parallel processing may be advantageous. Moreover, the separation of various system components in the implementations described above should not be understood as requiring such separation in all implementations, and it should be understood that the described program components and systems can generally be integrated together in a single product or packaged into multiple products.

A number of embodiments have been described. Nevertheless, it will be understood that various modifications can be made. Accordingly, other embodiments are within the scope of the following claims. 

What is claimed is:
 1. An integrated quantum circuit, comprising: a first substrate comprising: a first surface, a recess formed in the first substrate along the first surface and having a recess surface, the recess configured to enclose a quantum circuit device, and a first electrically-conductive layer disposed on the first surface and covering at least a portion of the recess surface, the first electrically-conductive layer comprising a first superconducting material; and a second substrate, comprising: a second surface, the quantum circuit device, disposed on and contacting the second surface, and a second electrically-conductive layer disposed on the second surface and comprising a second superconducting material; wherein the first substrate is disposed adjacent the second substrate to enclose the quantum circuit device within the recess of the first substrate; and wherein the first electrically-conductive layer of the first substrate is electrically-coupled to the second electrically-conductive layer of the second substrate.
 2. The integrated quantum circuit of claim 1, comprising a third superconducting material electrically-coupling the first electrically-conductive layer to the second electrically-conductive layer.
 3. The integrated quantum circuit of claim 2, wherein the third superconducting material is a bump.
 4. The integrated quantum circuit of claim 2, wherein the third superconducting material is a layer disposed over at least one of the first electrically-conductive layer and the second electrically-conductive layer.
 5. The integrated quantum circuit of claim 2, wherein the third superconducting material comprises indium.
 6. The integrated quantum circuit of claim 2, wherein the third superconducting material comprises gallium.
 7. The integrated quantum circuit of claim 1, wherein the first electrically-conductive layer is a multi-layered stack in which one layer is formed of the first superconducting material.
 8. The integrated quantum circuit of claim 7, wherein the multi-layer stack comprises: a first layer formed of the first superconducting material; and a second layer in contact with the first layer and formed of non-superconducting material; wherein the second layer is sufficiently thin such that, when the first layer becomes superconducting, the second layer becomes superconducting via a proximity effect.
 9. The integrated circuit of claim 7, wherein the multi-layer stack comprises: a first layer formed of the first superconducting material; a second layer in contact with the first layer and formed of non-superconducting material; and a third layer in contact with the second layer and formed of superconducting material; wherein the second layer is sufficiently thin to allow superconducting electrical signals to be exchanged between the first layer and the third layer via a proximity effect.
 10. The integrated quantum circuit of claim 1, wherein the second electrically-conductive layer is a multi-layered stack in which one layer is formed of the second superconducting material.
 11. The integrated quantum circuit of claim 10, wherein the multi-layer stack comprises: a first layer formed of the second superconducting material; and a second layer in contact with the first layer and formed of non-superconducting material; wherein the second layer is sufficiently thin such that, when the first layer becomes superconducting, the second layer becomes superconducting via a proximity effect.
 12. The integrated quantum circuit of claim 10, wherein the multi-layer stack comprises: a first layer formed of the second superconducting material; a second layer in contact with the first layer and formed of non-superconducting material; and a third layer in contact with the second layer and formed of superconducting material; wherein the second layer is sufficiently thin to allow superconducting electrical signals to be exchanged between the first layer and the third layer via a proximity effect.
 13. The integrated quantum circuit of claim 10, wherein the second superconducting material is titanium nitride.
 14. An integrated quantum circuit, comprising: a first substrate comprising: a first surface, a recess formed in the first substrate along the first surface and having a recess surface, the recess configured to enclose a quantum circuit device, and a first electrically-conductive layer disposed on the first surface and covering at least a portion of the recess surface, the first electrically-conductive layer being a multi-layered stack that comprises: an inner layer in contact with the first surface of the first substrate and formed of niobium, the niobium being a first superconducting material, and an outer layer formed of an alloy of molybdenum and rhenium; and a second substrate, comprising: a second surface, the quantum circuit device, disposed on the second surface, and a second electrically-conductive layer disposed on the second surface and comprising a second superconducting material; wherein the first substrate is disposed adjacent the second substrate to enclose the quantum circuit device within the recess of the first substrate; and wherein the first electrically-conductive layer of the first substrate is electrically-coupled to the second electrically-conductive layer of the second substrate.
 15. The integrated quantum circuit of claim 14, wherein the multi-layer stack further comprises: a first intermediate layer and a second intermediate layer sandwiched between the inner layer and the outer layer; wherein the first intermediate layer is in contact with the inner layer and formed of an alloy of titanium and tungsten; and wherein the second intermediate layer is in contact with the first intermediate layer and the outer layer and is formed of niobium.
 16. An integrated quantum circuit, comprising: a first substrate comprising: a first surface, a recess formed in the first substrate along the first surface and having a recess surface, the recess configured to enclose a quantum circuit device, and a first electrically-conductive layer disposed on the first surface and covering at least a portion of the recess surface, the first electrically-conductive layer comprising a first superconducting material; and a second substrate, comprising: a second surface, the quantum circuit device, disposed on the second surface, and a second electrically-conductive layer disposed on the second surface, the second electrically-conductive layer being a multi-layered stack that comprises: an inner layer in contact with the second surface of the second substrate and formed of niobium, the niobium being a second superconducting material, and an outer layer formed of an alloy of molybdenum and rhenium, wherein the first substrate is disposed adjacent the second substrate to enclose the quantum circuit device within the recess of the first substrate; and wherein the first electrically-conductive layer of the first substrate is electrically-coupled to the second electrically-conductive layer of the second substrate. 